F-V & T-V

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  • Two types of electrical analogous1.Force-voltage analogous2. Force- current analogous1.Voltage source2.Current source

  • 1.F-V analogous 2. F- I analogous

  • F-V ---F-I & T-V ---T-I

    MECHANICAL Translational F-V (Mesh)F-I (Node)MECHANICAL RotationalT-V (Mesh)T-I (Node)Force-F(i/p)e or viTorque- T (i/p)e or viX or V (o/p)q or iV or or (o/p)i or qV or Mass MLCMoment of inertia JLCDash pot BR1/RDash pot BR1/RSpring K1/C1/LSpring K1/C1/L

  • Step -1Free body diagram of M1Step-2Opposing force acting on M1Step-3Newtons 2 nd law

  • Step -4Free body diagram of M2Step- 5Opposing force acting on M2Step- 6Newtons 2 nd law

  • Force - voltage analogous circuitOn replacing force elements by electrical voltage elements in eqn (3) & (4)

  • Force - voltage analogous circuit (mesh basis)From eqn (5) & (6) ,we get

  • Force - Current analogous circuit (node basis)On replacing force elements by current elements in eqn (3) & (4)

  • From eqn (7) &(8)Force - Current analogous circuit (node basis)V1V2

  • Step -1Free body diagram of J1Step-2Opposing Torque acting on J1Step-3Newtons 2 nd law

  • Step -4Free body diagram of J2Step-5Opposing Torque acting on J2Step-6Newtons 2 nd law

  • Step -7Free body diagram of J3Step-8Opposing Torque acting on J3Step-9Newtons 2 nd law

  • On replacing Torque elements by V elements in eqn (4) , (5) & (6)

  • On replacing Torque elements by I elements in eqn (4) , (5) & (6)

  • V1V3V2

  • *****


F Inal Mobile T V

F Inal Mobile T V

MALAYALAMprospectus 2019 20 FINAL · ï ®v£= f v ¹ v= F 9 t

MALAYALAMprospectus 2019 20 FINAL · ï ®v£= f v ¹ v= F 9 t

F A C T v s . M y t h

F A C T v s . M y t h

Annexe 2 -F-T-V-B

Annexe 2 -F-T-V-B

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F g g t v McGill University

F g g t v McGill University

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TO - DTIC · By f uthnr;t r-: |W«v \ «AHk n nm^V^V^S^T ^

TO - DTIC · By f uthnr;t r-: |W«v \ «AHk n nm^V^V^S^T ^

Real-time Atmosphericdeveloper.download.nvidia.com/presentations/2007/D3DTutorial_Cryt… · be d d d f v t dt f o td o td o td d dt v t o td f x y z be z z v v v v v v v −∫ −

Real-time Atmosphericdeveloper.download.nvidia.com/presentations/2007/D3DTutorial_Cryt… · be d d d f v t dt f o td o td o td d dt v t o td f x y z be z z v v v v v v v −∫ −

Amtliche Bekanntmachung - Universitätsklinikum Magdeburg1_Formblatt.docx · Web viewn s t a n t ritt) K a t e gor i e F: V o t um K a t e gor i e F: V o t um K a t e gor i e F: V

Amtliche Bekanntmachung - Universitätsklinikum Magdeburg1_Formblatt.docx · Web viewn s t a n t ritt) K a t e gor i e F: V o t um K a t e gor i e F: V o t um K a t e gor i e F: V

1 · V--:= .. Q,E 2.. f;, Wq"(,LL·~f.'''''·1'~·J. R:'kowl"~ V~c\~~.. T (-r), t o (~) • ---.. L~ v. k,.,

1 · V--:= .. Q,E 2.. f;, Wq"(,LL·~f.'''''·1'~·J. R:'kowl"~ V~c\~~.. T (-r), t o (~) • ---.. L~ v. k,.,

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T V)LNT F C TION

T V)LNT F C TION

~?V»~~~~~~~M~f]~' i;t»~~

~?V»~~~~~~~M~f]~' i;t»~~

Chapter 24 Wave Optics. General Physics Review – waves T=1/f period, frequency T=1/f period, frequency v = f velocity, wavelength v = f velocity, wavelength.

Chapter 24 Wave Optics. General Physics Review – waves T=1/f period, frequency T=1/f period, frequency v = f velocity, wavelength v = f velocity, wavelength.

F N T 'T kS A, Lufdcimages.uflib.ufl.edu/UF/00/00/15/65/14772/00024.pdfM INA I INT(TATRO Y11,p(01 1), A A N N C 1 0 S I C A 1) V F N T 'T V I N T A V F i S V E NTA V E N T A h: t.'

F N T 'T kS A, Lufdcimages.uflib.ufl.edu/UF/00/00/15/65/14772/00024.pdfM INA I INT(TATRO Y11,p(01 1), A A N N C 1 0 S I C A 1) V F N T 'T V I N T A V F i S V E NTA V E N T A h: t.'

Oscillations and waves. Simple Harmonic Motion - Kinematics = 2 f = 1 = 2 f T T x = x o sin( t) or x o cos( t) v = v o cos( t) or -v o sin(

Oscillations and waves. Simple Harmonic Motion - Kinematics = 2 f = 1 = 2 f T T x = x o sin( t) or x o cos( t) v = v o cos( t) or -v o sin(

O F F I C E O F T H E P R O V O S T

O F F I C E O F T H E P R O V O S T

x) · cot x = ¯csc 2 x d dx sec x = sec x tan x f(t) = 1 2 gt 2 + v 0 t + s0 v(t) = f'(t) a(t) = v'(t) = f"(t) d dx csc x = ¯csc x cot x d dx (f(x)⋅g(x))= f(x)g'(x)+ g(x)f'(x)

x) · cot x = ¯csc 2 x d dx sec x = sec x tan x f(t) = 1 2 gt 2 + v 0 t + s0 v(t) = f'(t) a(t) = v'(t) = f"(t) d dx csc x = ¯csc x cot x d dx (f(x)⋅g(x))= f(x)g'(x)+ g(x)f'(x)