AIEEE 2012 solution (26th may)
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Transcript of AIEEE 2012 solution (26th may)
Detailed solution given below Q1
1)
2)
3)
4)
ans 1 Q2
1)
2)
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4)
ans 4 Q3
1)
2)
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4)
ans 4
Q4
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ans4 Q5
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ans2 Q6
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ans1
Q7
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ans1 Q8
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ans4
Q9
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ans2 NOTE- actual ans is 0125m Q10
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ans3
Q11
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ans1 Q12
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ans2 (actual ans is 8888)
Q13
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ans3 Q14
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ans1
Q15
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ans3 Q16
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ans4
Q17
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ans4 Q18
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ans3
Q19 1)
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ans2 Q20
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ans3
Q21
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ans4 Q22
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ans3 Q23
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ans2
Q24
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ans4 Q25
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ans4
Q26 1)
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ans3 Q27
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ans2
Q28
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ans2 Q29
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ans3
Q30 1)
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ans2
Q61
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ANS1 Q62
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ANS3
Q63
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ANS 4 Q64
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4)
ANS2 Q65
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ANS4
Q66
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ANS2 Q67
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ANS4 Q68
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ANS3
Q69 1)
2)
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4)
ANS1 Q70
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ANS3 Q71
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4)
ANS2
Q72 1)
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ANS2 Q73
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ANS4 Q74
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4)
ANS1
Q75 1)
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4)
ANS1 Q76
1)
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ANS2 Q77
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ANS1 Q78
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ANS4
Q79
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4)
ANS3 Q80
1)
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4)
ANS2 Q81
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ANS4
Q82
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4)
ANS (ans is 4) Q83
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ANS3 Q84
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ANS4
Q85
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ANS1 Q86
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4)
ANS1 Q87
1)
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4)
ANS4
Q88 1)
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ANS3 Q89
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ANS4 Q90
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ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q4
1)
2)
3)
4)
ans4 Q5
1)
2)
3)
4)
ans2 Q6
1)
2)
3)
4)
ans1
Q7
1)
2)
3)
4)
ans1 Q8
1)
2)
3)
4)
ans4
Q9
1)
2)
3)
4)
ans2 NOTE- actual ans is 0125m Q10
1)
2)
3)
4)
ans3
Q11
1)
2)
3)
4)
ans1 Q12
1)
2)
3)
4)
ans2 (actual ans is 8888)
Q13
1)
2)
3)
4)
ans3 Q14
1)
2)
3)
4)
ans1
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q7
1)
2)
3)
4)
ans1 Q8
1)
2)
3)
4)
ans4
Q9
1)
2)
3)
4)
ans2 NOTE- actual ans is 0125m Q10
1)
2)
3)
4)
ans3
Q11
1)
2)
3)
4)
ans1 Q12
1)
2)
3)
4)
ans2 (actual ans is 8888)
Q13
1)
2)
3)
4)
ans3 Q14
1)
2)
3)
4)
ans1
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q9
1)
2)
3)
4)
ans2 NOTE- actual ans is 0125m Q10
1)
2)
3)
4)
ans3
Q11
1)
2)
3)
4)
ans1 Q12
1)
2)
3)
4)
ans2 (actual ans is 8888)
Q13
1)
2)
3)
4)
ans3 Q14
1)
2)
3)
4)
ans1
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q11
1)
2)
3)
4)
ans1 Q12
1)
2)
3)
4)
ans2 (actual ans is 8888)
Q13
1)
2)
3)
4)
ans3 Q14
1)
2)
3)
4)
ans1
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q13
1)
2)
3)
4)
ans3 Q14
1)
2)
3)
4)
ans1
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q15
1)
2)
3)
4)
ans3 Q16
1)
2)
3)
4)
ans4
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q17
1)
2)
3)
4)
ans4 Q18
1)
2)
3)
4)
ans3
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q19 1)
2)
3)
4)
ans2 Q20
1)
2)
3)
4)
ans3
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q21
1)
2)
3)
4)
ans4 Q22
1)
2)
3)
4)
ans3 Q23
1)
2)
3)
4)
ans2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q24
1)
2)
3)
4)
ans4 Q25
1)
2)
3)
4)
ans4
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q26 1)
2)
3)
4)
ans3 Q27
1)
2)
3)
4)
ans2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q28
1)
2)
3)
4)
ans2 Q29
1)
2)
3)
4)
ans3
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q30 1)
2)
3)
4)
ans2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q61
1)
2)
3)
4)
ANS1 Q62
1)
2)
3)
4)
ANS3
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q63
1)
2)
3)
4)
ANS 4 Q64
1)
2)
3)
4)
ANS2 Q65
1)
2)
3)
4)
ANS4
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q66
1)
2)
3)
4)
ANS2 Q67
1)
2)
3)
4)
ANS4 Q68
1)
2)
3)
4)
ANS3
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q69 1)
2)
3)
4)
ANS1 Q70
1)
2)
3)
4)
ANS3 Q71
1)
2)
3)
4)
ANS2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q72 1)
2)
3)
4)
ANS2 Q73
1)
2)
3)
4)
ANS4 Q74
1)
2)
3)
4)
ANS1
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q75 1)
2)
3)
4)
ANS1 Q76
1)
2)
3)
4)
ANS2 Q77
1)
2)
3)
4)
ANS1 Q78
1)
2)
3)
4)
ANS4
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q79
1)
2)
3)
4)
ANS3 Q80
1)
2)
3)
4)
ANS2 Q81
1)
2)
3)
4)
ANS4
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q82
1)
2)
3)
4)
ANS (ans is 4) Q83
1)
2)
3)
4)
ANS3 Q84
1)
2)
3)
4)
ANS4
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q85
1)
2)
3)
4)
ANS1 Q86
1)
2)
3)
4)
ANS1 Q87
1)
2)
3)
4)
ANS4
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
Q88 1)
2)
3)
4)
ANS3 Q89
1)
2)
3)
4)
ANS4 Q90
1)
2)
3)
4)
ANS2 By Saurav gupta Electronics amp tele comm Engg (2nd year) Jadavpur university
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q1
Bqv= mvsup2R
R= mvBq
Now
eV= frac12 mvsup2
or mv= radic2emV
R= radic2emVBq
Rprop radicm
Rrsquo = radic2R
Ans -1
Q2 q1+q2 = Q ---eq(1) given
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
σ1=σ2--- given
or q14πrsup2=q24πRsup2
q1rsup2= q2Rsup2-------- eq(2)
solving eq (1) amp (2) we get
q1 =Q(1+rsup2Rsup2)
now
V=14πϵ˳ (q1r+q2R)
=14πϵ˳ q1(1r+ q1 Rrsup2)
=Q4πϵ˳ (r+R)(Rsup2+rsup2)
Ans -4
Q3 Sinα ≃ tanα≃α
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=dD
Δx=λdD dα
=λα D
Ans 4
Q4 E=[Ecosωt+Ecos(ωt) cos(ωt)]icirc
=[Ecosωt+E2cos(ω+ωt)
+E2cos(ω-ωt)]icirc
Ans 4
Q5 N MSD = (N+1) VSD
1 VSD = N(N+1) MSD
NOW
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
LC = 1MSD -1VSD
=[1 ndash N(N+1)]MSD
a(N+1)
Ans 2
Q6 Case1
Tension unit length = 100gl
Case2
Tension unit length= 2mgl
2m=100
m=50kg
Ans -1
Q7
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dqdt = dqdtˢ
9KA(100-θ)(L2)=KAθ(L2)
θ=90⁰
Ans -1
Q8 F = dPdt
=ddt(mv)
= v dmdt
= 6
Ans 4
Q9 s
τ=-mgsinθR
≃-mgθR
Iα=-mgθR
mgsinθ
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
α=-mgRθI
ωsup2=mgRI
now
I = mRsup2 + mRsup2
=2mRsup2
ωsup2=g2R
T=2πradic(2R)g
Putting T=1 amp g≃πsup2
R= 18
=0125
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q10 υn= (2n-1)v4L
case1
500 = (2n ndash 1)v4 x16 ----(1)
Case2
500 = (2nrsquo-1)v4 x 50-----(2)
Solving 1 amp 2 we get
50n -16nrsquo = 17
n≃1nrsquo≃2
now solving for v
v = 500 x4 x 503
v = 3333333ms
now
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
υ(fundamentaloutsidewater)=vλ
=v2l
≃276 Hz
υ(2nd lowest)=2υ
=552 Hz
Ans -3
Q11 λav= λα+λβ
now
Tfrac12=1λ
Tav=1λα+1λβ
Ans -1
Q12 Mu = mv + mvrsquo
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
frac12 musup2 = frac12 mvsup2 + frac12 mvrsquosup2
Solving eq (1) amp(2)
V = -13u
Vrsquo= 23u
(ΔEE)x100= 8888
Ans 2
Q13 Sinθ gt1μ
μgμw=15(43)
= 98
Sinθgt89
Ans 3
Q14
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
KE=hυ-hυ˳
IfυisdoubledKEismorethandoubled
Also
Photocurrent depends on intensity not on frequency
Statement 1- false
Statement 2-true
Ans -1
Q15 q(E + v x B)= 0
E = - v x B
E = B x v
E=E˳cos(wt-2πλy)ẑ
Ans -3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q16 I Esup3= 136 zsup2nsup2
= 136 x 9
= 1224
TE = IEsup1 + IEsup2 + IEsup3
=54 +756 +1224
= 2034
Ans 4
Q17 P=Vsup2R
R1ltR2
P1gtP2
Ans -4
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q18 H=Isup2Rt
ΔH=2ΔI+ΔR+Δt
= 6
Ans -3
Q19 vsup2 = usup2 + 2al
Vrsquosup2 = usup2 + 2a(l2)
=usup2 + frac12 (vsup2-usup2)
Vrsquosup2 = (vsup2 + usup2)2
Vrsquo = radic(vsup2+usup2)2
Ans -2
Q20 Statement 1 ndashtrue
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Statement 2- true
Bnearthecentreisμ˳nibutdecresesaswemovetowardsitrsquosendandbecomesμ˳ni2atthe extreme end which explains statement 1
Ans -3
Q21 V = e ndash iR
120 ndash 50 x 01
= 115
Ans 4
Q22 Y=Asin(ωt+2π3)
At t=0
Y = A sin 120⁰
Checking option
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans -3
Q23 Fsinθ
Fκ Fcosθ
Fκ = μ(mg- Fsinθ)
Now
Fcosθ = Fκ
F = μW(cosθ + μsinθ)---(1)
For minimum force
mg
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
dFdθ = 0
solving we get
tanθ = μ
or cosθ= 1radic1+μsup2
or sinθ = μradic1 +μsup2
substituting these values in eq ndash1
F = μWradic1 +μsup2
Ans -2
Q24
As we pull the connector by say x amount there will be growth in current in the circuit which will
be opposed by the inductor(due to self inductance)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Here inductor is analogous to spring(mechanical analog of inductor)
Opposing force prop -x
Hence the connector will execute SHM
Ans 4
Q25
P =αv
Vf= m Vᵢ
W = int p dv
= αintvdv
= α2 (vfsup2- vᵢsup2)
= αvsup2 (msup2-1)2
Ans -4
Q26
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ф = EA cos 45⁰
= E πasup2radic2
Ans -3
Q27
L = constant
Mvr = constant
fMr = (1-f)Mvrsquorrsquo
frsup2ω = (1-f)rrsquosup2ωrsquo
ωωrsquo = (1-f)f x (rrsquor)sup2---(1)
now
mr = mrsquorrsquo
fMr =(1-f)Mrrsquo
rrsquor = f(1-f)
putting this in eq ---(1)
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
ωωrsquo = f(1-f)
Ans -2
Q28
ᶯ(max) = 1- T2T1
= 1 ndash 273373
= 2680
Hence 30 efficiency is not possible by carnotrsquos theorem
Ans 2
Q29
Vol(initially) = vol(finally)
n 43 πrsup3 = 43 π Rsup3
n = Rsup3rsup3
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE PHYSICS SOLUTION (EXAM-26TH MAY 2012)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now
12mvsup2=Δs
= n 4πrsup2T - 4πRsup2T
Solving we get
Vsup2 = 8πTRsup2m [Rr -1]
Put m = ρ x 43 πRsup3
V = 6Tρ[1r -1R]⁰⁵
Ans- 3
Q30
Self explanatory
Ans -2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q61
Lt x-gt 2ˉ x[x] le limx-gt 2ˉ f(x) le lim x-gt2ˉ radic6-x
2 le limx-gt2ˉ f(x) le 2
Limx-gt2ˉ f(x) = 2
Statement 1---true
f(2)=1 ----given
Limx-gt2ˉ f(x) ne f(2)
Hence f(x) is not continuous at x=2
Statement 2- ----false
Ans 1
Q62
n(f) = ⁴C1 x 2 x 4
= 32
n(s) = 5 =120
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
p = 32120
= 415
Ans 3
Q63
g(x) = axsup33 + bxsup2 + cx
g(x) = axsup2 + bx + c
now
g(1)=0 g(x)= 0 and g(x) is obviously continuous
by rollersquos theorem
at some point between (01)
grsquo(x)=0
hence
axsup2 +bx +c = 0
has itrsquos root between (01)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q64
bsup2+csup2 ab ac
ab csup2+asup2 bc
ac bc asup2+bsup2
-asup2 ab ac
= ab -bsup2 bc
ac bc -csup2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
-1 1 1
= asup2bsup2csup2 1 -1 1
1 1 -1
= 4asup2bsup2csup2
Ans 2
Q65
2secθ = sec(θ+ф) + sec(θ-ф)
2cos(θ+ф)cos(θ-ф)
cos(θ+ф) +cos(θ-ф)
= (cossup2θ ndashsinsup2θ) cosθcosф
Cossup2θ(cosф-1) = -sinsup2ф
Cossup2θ = 2 cossup2ф
K= plusmnradic2
Cosθ =
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 4
Q66
M = L + (N2 ndash c)x hf
25 = 20 + (50-45) x 10f
F =10
Ans 2
Q67
Xsup2 + secsup2x -1
1+xsup2
Secsup2x (1+xsup2) -1
1+xsup2
intSecsup2x dx - int dx1+xsup2
F(x) = int
F(x) = dx
dx
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
f(x)= tanx ndash tanˉsup1x + c
f(0) = 0
C = 0
f(1) = tan1 ndash tanˉsup11
= tan1 ndash π4
Ans 4
Q68
dr of normal to plane 1 ---(100)
dr of normal to plane 2 ---(2-5a3)
dr of normal to plane 3 ---(3b1-3)
let dr of common line (pqr)
now
line is perpendicular to plane1
P=0-----(1)
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
line is perpendicular to plane 2
2p -5aq + 3r = 0----(2)
line is perpendicular to plane 3
3pb + q ndash 3r = 0----(3)
Solving these eq we get
a =15
Ans 3
Q69
lim f(1-α) ndashf(1)
α - 0 αsup3 + 3α
frsquo(1-α)
3αsup2 + 3
= frsquo(1)3
=
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
= -533
Ans 1
Q70
(x + 32)sup2 + ysup2 = (32)sup2---(1)
Y = mx+1---(2)
Solving eq (1) amp(2)
Ysup2(1 +msup2) - y(3m + 2msup2) +1msup2-3m = 0
Since two points are equidistant from and opp sides of x-axis
Sum of the roots of this eqᶯ must be 0
ie
3m + 2msup2 = 0
3m + 2= 0
Ans 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q71
θ π-θ
w = -a ndash ib
-w =a +ib
= z
Statement 1mdashtrue
Statement 2---false
As |z|=|w| only implies that they are equidistant from centre of argand diagram
Z=a+ib W= -a+ib
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q72
Pxsup2 + qx + r = 0
αβ = rp
let α= a+ib
then β=a-ib
αβ = asup2 + bsup2
|α| +|β| = radicasup2+bsup2 + radicasup2+bsup2
=2radicasup2+bsup2
=2radicrp
Since rgtp
|α|+|β|gt2
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q73
(01)
(a2a) Y=2x
(αβ)
(Y-1)x= (2a-1)a
Slope of this line m1= (2a-1a)
Slope of given line m2= 2
Since these lines are perpendicular
m1 x m2= - 1
we get
a = 25
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
now (a2a) are middle points of (10) and (αβ)
we get
α = 45 β = 35
Ans 4
Q74
sup2C1 x ⁴C2 x 3 + sup2C2 x ⁴C1 x 3
= 96
Ans 1
Q75
n p(s) = 2sup3
n(s) = 3
no of one one relation is ⁸P3 = 336
Ans 1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q76
Area= int x dy
=˳int⁸ ysup1 sup3 dy
= 12
Ans 2
Q77
P q = ~p v q
Basic formula
Can check it by truth table
Ans 1
Q78
Xsup2 = 8y
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
(Y ndash 2)= -dxdy|ˣ ⁴ (x-4)
y-2 =4-x
x +y = 6
Ans 4
Q79
|a+b| = radic asup2+bsup2+2abcosθ
|c| = radic 9+25+2x3x5cosθ
30cosθ = 15
θ= 60⁰
Ans 3
Q80
˳int⁰⁹ [x -2[x]] dx
[x] = 0 0lexle09
˳int⁰⁹ o dx = 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Ans 2
Q81
I F = exp( int 2x dx)
=xsup2
Now
yxsup2 = int xsup2xsup2 dx + c
y = xsup35 + cxˉsup2
Ans 4
Q82
bf-ec -ae -ab
Aˉsup1 = -1bd cd -ad 0
-bd 0 0
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
0 0 d
A = 0 b e
a c f
now
Amacrsup1 = A
comparing we get
c=0 e=0 f=0 a=1a=bsup2a=dsup2
or bsup2 =1 dsup2 =1
or b = plusmn1 d= plusmn 1
hence there are 4 possible matrices
Ans
Q83
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
N = 2tsup2 + 3 w = tsup2 -t +2
dwdt = n dwdt + w dndt
= 8tsup3-6tsup2+14t-3
dwdt|at (t=1) = 13
Ans 3
Q84
radic (x-1)sup2 + ysup2
radic (x+1)sup2 + ysup2
Solving we get
Xsup2+ysup2-103 x+1 = 0
Centre = (53 0)
Hence the circumcentre of the triangle is (53 0)
Ans 4
= frac12
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
Q85
Given lines
x2 = y-1 = z2
(x-1)4 = (y-1)-2 = (z-1) 4
These 2 lines are parallel
p(111)
line 1
q(2λ-λ2λ) line2
line pq and line(1 or2) are perpendicular
hence
(2λ-1)2 + (-λ-1)-1 +(2λ-1)2 = 0
λ = 13
q = (23-1323)
length pq = radic2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
statement 1----true
Ans 1
Q86
1 + 43 + 109 + helliphellip
1 +(1+13)+ (1 + 19) + hellip
n + (13 +19 + 127 +hellip)
n + frac12[1- 13ᶯˉsup1]
Ans 1
Q87
Foci of ellipse= radicasup2-bsup2
=radic16-bsup2
Foci of hyperbola = radicasup2+bsup2
=3
radic16-bsup2 = 3
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
bsup2 =7
Ans 4
Q88
Tanˉsup1(sin(cosˉsup1radic23))
Tanˉsup1(1radic3)
π6
Ans 3
Q89
c is perpendicular to a x b
c(a x b) = 0
1 -2 3
2 3 -1 =0
r 1 2r-1
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2
AIEEE 2012 ONLINE DETAILED SOLUTION (DATED 26TH MAY)
BY
SAURAV GUPTA
ELECTRONICS amp TELECOMM ENGG(2ND YEAR)
JADAVPUR UNIVERSITY
r= 0
Ans 4
Q90
n = m(m-1)2
n-1 = m(m-1)2 - 1
ᶯC2 = n(n-1)2
Solving we get
ᶯC2 = 3 ˉ sup1C4
Ans 2