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Transcript of Physics Preston Notes
8/6/2019 Physics Preston Notes
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gHAPTER
WAVES
tn Understandingaves1 An oscillatingystem uch sa simple endulumr a
loaded pring wingso and roabout fixed osition.AmplitudeA) s hemaximumisplacementinmeter)ftheoscillation.eriodT) s he ime insecond)akenocompletene ycle f heoscillation.requencyf) s henumberinHertz) foscillationshat ccurnoneperiod.
t 1Therefore, fT orT= r
2 A wavemotion s th ephenomenonf energyransferfacilitatedy heoscillationfmoleculesfamedium.f hevibrationf hemoleculessperpendicularo he irectionfthewavemotion,hewavescalled ransverseavesuch
aswaterwave).f themoleculesibraten parallelo thewavemotion,hewave sknown sa longitudinal ave(such ssound ave).
3 Graph shows displacement-distanceraph f a wavemotion. avelengthinm) s hedistanceccupiedyonecompleteycle f hewave.
DisplocementDistonce roph A)
Amplitude
(' )
DisplocementTimeGroph(B )
Amplitude
(m)
1 wove velocity= 2-r ms-r
Graph showsdisplacement-timeraph fawave.Wavevelocityinms-1)s henumberfwavelengthsor istance)thewave dvancesnone econd.
Wavelength, frequencyandwave elocityare elatedin hewaveormula: = l.A wavefrontsan maginaryurfaceoiningll hepointsnspacehatare eachedt th esame nstant y a wavepropagatinghrough medium.na plan iew, aves reoften epresentedn diagramsy a series f l ines fwavefront.hedirectionsf thepropagationf hewaveswhich re erpendicularo hewavefrontsre suallyhownassmall rrows.
l ml
i''l,on." 6
Wovefronts
Afterhe nitial isturbance,noscillationystem il leither
carry ncontinuouslyr slow own nd top ventually.n
the irst ase,he ystems n esonanceroscillatingt tsnaturalrequency. physicalystemmayhave everalnaturalrequenciestwhicht canvibrateasily ith erylittle dditionfenergyrom nexternalource. henevertvibratest oneof tsnaturalrequencies,t ssaido be n
resonance.n he ater ase,hephenomenons known sdamping hich suallyccursn hepresencef friction.
Frictioncts gainsthemotionndprogressivelyeduces
theosci l lat ionmpli tudelthoughhe requencyf hevibrationemainsnchanged.Phenomenauchas reflection,efraction,iffractionndinterferencereobservedhen wavemeets nobstacle
orawavemeets ther aves.he ules fsuch henomenareapplicableo all ransversend ongitudinalavesincludingight,ound ndwater aves.
@ Analysing eflection
1 The awof reflectiontateshat heangle f ncidenceequalso heangle f eflection.Examplesf eflection:
Incidentolwoves
Normql
; reflected woves- - J - - -
I
The requency,avelengthnd peed f hewave emainthesame fterhe eflection.owever,hedirectionf hewavewillchangend hereforehevelocity illalso ifferafterhe eflection.
(s)
Time
. r m
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tf,l Analysing efraction
1 The efractionf waves anbedemonstratedna rippletank ychanginghewater epth tvariousegionf hewaterank.When ater avesravelrom deeperectiontoa shallowerection,t s efracted.hewaves ovelowlyinshallowaternd he eductionfspeedauseseductioninwavelengthhi lehe requencyemainsnchanged.
Wavefrontslose pon each ther nd hewaves en dtowardshenormalf he ntersection
4 Variousiffractionatterns:
2
@ Analysing iffraction
Th e henomenonfdiffractionccurshen ither smallobstacleranobstacleith narrowpeningsplacedn
thepath fprogressingavesna rippleank. he ffect fdiffractionssignificantnlywhenhe ize f heobstaclerthegapof heobstaclesvery mallncornparisono hewavelengthf h ewaves,The requency,avelengthnd peed f hewavesemainthesame fterhediffraction.owever,hedirectionf hewaves ill hangend hereforehe elocityil l lso ifferafterhediffraction.hewaves pread utas hey ass
through narrow apand hereforeheshape f thewavefrontshangesfterhediffraction.Lightsalso iffractedhent spassedhroughnarrow
slit. ut he ffectsonly oticeablehe nhe li twidthsnomorehan ne-hundredthfamillimetersuggestinghatightsarewaves ith erv hortwavelenoth.
- f
'.r
t-+
}.
i - - - 2
Variousxamplesf efraction:
3F| Analysingnterference
1 Interferenceccurs' ,- :- , ' , - ' - - ' . , ' ,, :s
t h e s a m e m e d i u mt ' : : = - . : - : ' - =. ' , , =i .e.hey avehe arr ie-i : -=- . . . . : :- : ' .
complexpat ternf rr - ' .? ' - : : - : . - - .
p r i nc i p l ef superpos i t i on: : : ' - :
t h roughach the r' , ^ : - : : - : : : ' -
d isplacementofheme: - = ' - . : . - " -
s imp l y theum f he : . : - : : : : : :2 Anexper imentnownsYc. ' : s : : - :
can e arr iedut ode-: -: : '=:
lf he istanceehvee'perpendicularistar:nodes.hewavelencr:
o fampl i tudehi le i r : - . : . , - : " : -
t h e y a n c e la c h t h e r : - : : ' , : - : -
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fE| UnderstandingoundWaves
Sound aves hich re ausedyvibrationsfasubstance,.g. speakerone, re ongitudinalnnature.hemoleculesfai rwobblenadirectionarallelo he irectionf he ravelingound.ound av e eedsmediauchasair,water nd oncreteo ravelhrough.tcannoto hroughvacuum here edia onotexist. 66$eedofsoundnvariousediaiffers.ts peedndry ir at oc),inwaterat0'c)an dnconcretere 00ms-1,1400s- land5000ms-1 espectively.Differentrequenciesoundifferento he ar . ighrequenciesre eardshigh itch otes hileow requency
soundsre aidobeof ow itch.ound aves ithargemplitudeppearobe oud n he arwhileoundshichhave mall mplitudere aidobesoft.Reflectionrecho fsoundrovideswa yomeasureistance.he quations
(speedfsound)= 26 (twicehedistanceromhe ourceo he eflection)t (theimehe oundakeso ravel acko he oure,e)
Gl Understandinglectromagneticaves
The lectromagneticpectrumsa continuousequencefall nownypes felectromagneticadiation,rrangedbywavelengthangingrom he hort osmicayshroughammaays, -rays,ltravioletadiation,isibleights,infraredadiation,icrowaves,o he ongwavelengthsf adio aves.Electromagneticaves ave roperties
uch swavelength,mplitude,requencyndpower.hey reelectric,magneticnd ransversennature.hey an ravelhroughree pacenstraightines ta speedfapproximatelyx 108ms-1(commonlynowns he peeof ight).he nergyfanelectromagneticaveadiatingrom sourcediminishess t ravelsutwardsnd s nverselyroportionalo he quaref tsdistanceromhesource.Wavelengths,ypes ndheirespectivepplications:
Wavelengthm) 104o3 x 10-1m 10r to 3 x 10-1m 10{ o10rm 4 x 10'7o7 x ' 1 0 tm
TypesfWaves Radio aves adio, Microwave Infrared Visibleights
Applications TV elecommunicationselecommunications,i'adar,ookingven
Thermography,night ision,eatingdevice
Vision,hotosynthesis,photography
Wavelengthm) 104o10rm 10-11o104m 10-14o 10-11
TypesfWaves Ultravioletights X-rays Gammaay s
Applications Moneynspection,terilisation,pesterminator
Radiography,adiotherapy,wieldingnspection
Destroyancerell, terilisation,Pesterminator
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gHAPTER
ELECTRICITY
123
4
5
67
@ Analysing lectricFieldsand ChargeFlowBasicallyhere re wo yp es f electricharges:+)positivehargend -)negativeharge.TheS.l, nitorelectrichargesCoulombC) .The hargefa protonspositive+1.6 10-1e)and he hargefanelectronsnegative-16x 10-1e).Aneutronas ocharge0C)and sconsideredeutral.nobject hich as higherumberfelectronsil lthereforeea negativelyhargedbject. ome bjects hen ubbedose rgain lectronasily nd husbecomeegativelyhargedrpositivelyhargedfterubbingit h notheratedal.Eiectricurrentepresentshemovementfelectrichargesndsdefineds he ate f low felectricharge.
The ormulaor urrentI) s =f wnere s he uantity
ofchargenCoulombnd is he ime urationnSecond.TheS.l. nitor urrentsAmpereA) nd A= 1Cs-1.Ina solidonductor,lectronsre lowingromhe egativeerminalo he ositiveerminal.ut yconvention,th e irectionf currentlow sconsideredlowingro mhepositiveo henegative.
8 Electrichargesnteractit h ac h ther.ike hargesepel hile nlikehargesttract.ines f orce rawnfrom ositivehargeo negativehargesusedo representuc hnteraction.nan areawhereheres adistributionfelectricharges,uchines f orceorm nelectricield. he ines fanelectricield i l l rovidean ndicationf he ath fa positivehargef t s reeomoven he ield.
9 Examplesfelectricields:
Effect f e lectr icie ldon chorge ing-pong ol lexperiment.
(o) (b )
r=t 7- F.t u \ Fll-6. ll l,l ,brll - l -F l * l I - l F : l * ll - I l + l l - | l + l? . - - r - + +
l - + l l - + l+H .V .+ +H.V.+
Effect f e leclr icie ldon chorge ondle lome.
(.) l-+l Fl+ 597/l-l
l l lKryt-tl * l J ( l - lf / \ i
Tl + l+ H . V . +
13
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CurrentandPotentiatDifference
1 Potentialifferencep.d.)etween'twoointsnanelectric
fields hework eededomove unit hargerom ne oint
toanother.2 Theormulaorp.d.(V)sV= { wnereW s hework one
inJoule ndQ squantityfchirgenCoulomb.
3 TheS.l.unitorpotentialifferencesVolt V)and1V=1JC-1.
4 Ohms aw tateshattheotentialnergyV) crossmetal
conductorsdirectlyroportionalo thecurrentI) lowing
@ Analysing elationshipetween
O K Tc Temperoture
throught providedhe emperaturend ther hysical6p Analysing Series and parallel
conditionsemainonstant:Circu i ts
1 The esistorsn heFigurere onnectednseries.
+ V r - + V z - + V s -
The .l. nitor esistancesOhm A)and Oh m 1VA-1.Factorsffectinghe esistanceR)of a conductornclude
its ength/) , tscross sectionalrea A) , tsmaterial
(resistivity)andts emperature0).p =O*
q)()o.2
o)E
i.e. - | or L =constant.I
5 The onstantf ) .nrtsentshe ppositionf he onductor
materialo he lectricurrentlow ndsgiven name alled
Resistance.he ormulaorResistanceR)sR=f
where
V sp.d.nVolt nd scurrentnAmpere.
67
R{O ) R ei)
L,(,,.inLf,,^.,tR (O )
(current)
1,.l./(
-]----------------- Temperorure' 0fc)
The esistancef a conductoril ldrop n andem ith tstemperature.he esistancefsomematerialsil l venal l
tozerowhents emperatures oweredo a certainegree.Suchmaterialsre alleduperconductors.ecausefzeroresistance,lectricalunent ill loworeverna closedooponcet sset nmotion.
The ame urrentlowshroughach f he esistors.l = 1 , , = l r = 1 ,Th e um f he .d. crossachesistorqualso he .d. fthe ource. =V,+V2+ 3Th e ombinedesistancef he esistorsnseriesqualsothe um f he esistancefall he esistors.= R,+ R,+ Rr .Th eeffectiveesistancencombinatrons hereforelargerha nhe esrstancefeachesistorn tsown.The esistorsn heFigurere onnectednparallel.
The ame .d.sactingOol'r..ur.nf he esistors.=Vr=
Vr=V,The urrentfromhesourcequalso hesum fcurrentsflowingneachesistor.= ,+ r+ ,The eciprocalf he ombinedesistancef he esistorsinparallelequalso he um
f he eciprocalsf he esistance1 1 ' l , Iof eachesistor.R-
=Ri
*R;
*R; . Theeffective
resistancen combinations thereforemallerhan heresistancefeach esistorn tsown.
Superconduc 'c .
;T l+ Y t -
, R : tL------:____l
+ V r -
t4
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@ Analysing lectromotiveorceand nternalResistance
Electromotiveorce re.m.f.nshorts hepotentialfanelectricourceomove lectrichargeshroughcompletecircuit.he .m.f. f he ourcendicateshe otal nergyhesourcescapablefgivingoeach nit harge.lnternalesistancef a cellor an electricource xists
becausef hepropertiesf tselectrolytend/ortselectrodeconnections.henternalesistancesusuallyuiteow;e.g.about .5Ohmsora dry ell.Owingo heeffect f he nternalesistance,hep.d. crosstheerminalsfacellwillvaryn elationo he oad onnectedto t. nanopen ircuit,heresno oad ndnocurrentlow,thep.d. crosshe nternalesistanceszero nd ence.dacrosshe erminalqualso hee.m.f. f hecell.n hecase fa oad,herescurrentlowesultingcertainmountofvoltagerop crosshe ntemalesistance.encehe .d .acrosse erminalil l e owerhanhee.m.f.f he ell.RefertoheFigure,=E I rwhere s he .m,f., s hep.d.
crosserminals,is hecurrentlowingnd is heinternalesistance.
i - - - - -- - - - - r
ffil Anatysing lectricalEnergyand
Power1 Electricalnergys heelectricalotentialnergyained
byachargenanelectricource.scurrentlowshroughload,heelectricalotentialnergyf he harge ill e ostandsconvertedootherorms fenergyuch sheat,ightor sound. he ate twhich uch nergyransformationstakinglacesdefinedsElectric ower.
2 The ormulaeorelectricalnergyE)and lectricowerP)are espectively:E =VQwhere s he .d.nVolt, s he uantityfcharge
inCoulomb
P =
+
whereis he ime urationnSecond
34
TheS.l.unitof Electdc owersWaft W)and1 Watt=1 Js-1.Theunit fenergy easurementsed yTNB orelectricalconsumptionsKilowatt our kwh).On e ilowatt-hoursinequivalenthe nergyuppliednone ouroanelectricalappliancehose owersonekilowatt.rom 006 une,TNBschargingrate f 21.8 ents erunitor he irst 00units. ate f28.9 entser nit ill e hargedor nit 01to 1000 ndwhen onsumptionxceeds000 wh,31,2
cents ill e eviedneach nit.Typicalomesticppliancesan d heir lectricalower)inc lude:nergy-saveright u lb 17W), ungstenu lb(40-100 ), luorescentube 2040W), adio10W),fan 60W), V 80-140 ), ridge100-130),d t npair-conditioner800-950), ice ooker500-800)"andaterkettle2000W).Efficiency"r)ofanelectricalpplianceanbedefineds
useful nergyutput./
't-l=
T =
total nergynput
usefulowerutput
x 100%
x 1 0 0 %
of
o
total owernput
An energy-saveright ulb s more nergy ff ic ientncomparisono a tungsten-f i lamentight ulb ecausetrequiresess nergynputoproducenequal mountfl ight.
7 Ways o i nc rease f f i c i encyn domes t i cne rgyconsumption:a) Switchtof fwhen ot nuse. se imerfpossible.
b) Doenergyfficiencyomparisoneforeurchase.electonewitha size/capacityhatmeets ournormal eed.Useenergy aving lternative s;.g. luorescentubeinsteadf ungstenulb nd olar oweredeaternstead
ofelectricaleater
c) Avoid xcessivesageuch ssettinghermostatfair-conditionerr efrigeratortveryow emperature.
d) Keep ppliancesngood ondition;.g, leanilter ndreplacerokenoor eal.
e)Avoid astage;.g. oil namounthat ou eednsteadof a fullkettle r avoidrequentpeningf refrigeratordoor rprovideoodnsulationorair-conditionedoom.
15
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gHAPTER
ELECTROMAGNETISM
m Anatysinghe Magnetic ffectof a Current-carryingConductorAnelectromagnetsa emporaryagnetausedy urrentlowingna conduc-tor.The atternsfmagneticield roCucedycurrent-carryingonductorsependon he hape f he onductorssshownnFrgureelow.
(o )A long t ro igh t i re (b)A s ing leoop (c )A solenoid
The ight-handrip ule tateshatf he ight and rips coi l fwire i thhefingersn he irectionf he urrentlow,he humb il l ointo he orth ole fth eelectromagnet.The trengthfmagneticield fanelectromagnetncreases,vitha) he umberof urnsn hecoil,b)a largerurrentnd c) he ype f core uch s ron,ferromagneticaterial.
5 Appl icat ionsf electromagnetncludeagneticelay,lectr icel l , ar ieceand ircuitreaker.
ff,| Understandinghe Force n a Current-carryingConductor n a MagneticField1 When nelectromagnetsplacedear magnet,he nteractionf womagnetic
fields roducesorce n he onductorsshownnFiqureelow.
ht
ffi@-'l
Fleming'seft-handule tateshat f he humbnd irstwo ingersf he eft-hand reheld tright ngleo each ther,he humb iveshedirectionf heforce,he orefingerhowshedirectionf magneticield nd hemiddleingerpointsn hedirectionfcurrent.Themagnitudef he orcencreasesit h(a) he trengthf hemagneticield,(b) he ize fcurrentnd(c) he engthf he onductor.
26
4 Asimple.C. otornFigureelow
showshe urningffectfa coupleor wo ppositeorcesctingn wosidesf he oi l inhemaqnet ic f ie ld.
5 Thes p e e d f ro ta t i on f a D .C .motora' :e a' . . ' . : cvchanginghe
force f :^e : : - : e ihestrengthf
rnagnet ice a ' . 'eS:Ze fcurrentr
the engt r ' : 'e :c , or he urn ing
effect\ \ 'c: ' ' :^e c i t
, 3
Commulo t o r
f f , | Anaiysing lectro-magnet icnduct ion
M a g n e t i c n d u c t i o n s t h ep h e ^ : - e ' c ^ l n a t a r e l a t i v e
A ' ^ A I T A Ar r v ! E s . - s . , , s c l ' a W I f ea n O a
magnei 'e 'J producesne.m. f .ni h o , . o
Nlag, ie:' l - : t on scausedYchangen nemagnet icluxonacondr, lc tornd tsmagni tudethe,ncjuced- f ) ncreasesitha)herate fchangef hemagneticlux,(o he irengthf h emagneticieldand c) he engthf he onductor.Fa raday ' saws ta tesha t heinduced.m. f .n a conduc torsdirect lyroport ionalo the ate twhichheconductoruts hrough
l ines f h emagneticield.Lenz's aw tateshat he nducedcurrentlwayslowsna directionsuchha ttopposeshe hangeha tiscausingt.Fleming'sight-handule tatesthat f the humb nd irst wo ingersof the ight-handreheld t r ight
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l A
angleo each ther, iddleingerpointsn he irectionf h e nducedcurrent,he oref ingerhowshedirectionf magneticield nd hethumb iveshedirectionf he orce.App l i ca t ionsf e l ec t romagne t ici nduc t i onnc lude.C. ndD.C.generatorshichonvertechanical
energynto lectricityy he otationofconductoroilsnamagneticieldas shownn Figurea)and b)asshownelow.
A s imp le .C.genero tor
Adirecturrentlwayslowsnoned i r e c t i o nn d t h a s c o n s t a n ta m p l i t u d eh i l e n a l t e r n a t i n gcu r ren t l ows n twooppos i tedirectionslternativelyta constant
frequency.The mplitudefanA.C. oltageanbespecifiedn hree ays:(a)peako peak V* o valuee-
tween aximumndminirnum);(b)peakV^ value etweenaxi-
mum nb ero);nd(c) oot-mean-squar€V,,". hich
giveshe ame mountfpowertransfersa D.C. f th esamev a l u e ) . V 2 x V a n d V =
V ' P ' P P r ' m . s .p
\T
h e
O f
\ / o
a
i n
n
U J
v
ane
d
h eI J
^ +
g n
ffil AnalysingTransformers
1 Mutualnductions he lectromag-neticnductionf a coi lwhent splacedearoanotherhichas nalternatingurrentlowingn t .
A s imp le .C.genero tor
In dealransformer,=.
Vo--N; '
V"l.= ^l^ nd tsefficiencys s P Pv l
- l l . ' o / , , P P= 1 U U % rv t
= 1 0 0 % .
A transformeronsistsfaprimary
coi l nda secondaryo i lwoundaroundcommonore hichasses
the lux rom heprimary oil oandthroughhe econdaryoil.A step-downransformerasahigherumberf u rnsNo)n tsprimaryoilandan nput oltageVo)
willproducelower utputoltageat ts econdaryoi lwhi lestep-uptransformeras higheru,mberfturnsN,) nsecondaryndalsoh ighe ru tpu to l t ageV" )n t ssecondarvoil.
Mos t l ec t r i c i t ys p roducedygenera to rsr i ven y ro ta t i ng
turbines hichmay e urned ys team.wa te r .w ind o r o the rintermediatenergyarrier.A ransmissionystem onsistsf(a)a first tage fvery igh oltage
overheadinesve ron g istancee-
tween tep-upransformerst thepower lant nd heNationalr idNetwork,b)severalntermediatestagesrom heGrido substationsthrou h step-downransformersndoverheadablesnd c) as t tage
of distributionhichs hedeliveryfrom ubstationso heconsumersthroughverheadr undergroundcables.I n p o w e rr a n s m i s s i o n ,. C . sp re fe r red ve rD.C.because
transformersanbeusedoobtainhigh ol tagesor hepurposefachievingmallerurrentlow ndlowernergyossn he ransmssioncables.Most f hepowereneratedn hecountrys suppledo heNationalGridNetwork ith hepurposefbetterontrolnd igherfticiencyndistr ibut ionndalsomore el iablesupplyn heevent fa local lantfai lurermaintenance.
Shortagesf energyuels reateeconomicndpol i t icalr is is hichaffecthe ifeof everyonendherebymake s ealizehe mportancefarenewablenergyource.The mpactshat r imaryower
olants ave n theenvi ronmentinc lude(a) uclearowerlantsollutinghe
a tmosoherei th ad ioac t i venucl ides,
(b) ossil-fueledlantsausingcidrain nd lobalarmingnd
(c)hydroelectr icams rast ical lyalteringandscapend cologyflife vstems.
I n p r a c t i c e ,n e r g y o s s i n
transformersccursue o oartialf luxinkagen he oi lsnd lso eatlossrom onductoresistance,romeddy urrentndmagnetizationnddemagnetizationf he ore.Ways o improverans fo rmereff ic iencynclude(a ) singhickeroi l ir eo owerhe
resistance,(b)usinghin heetsf aminated
coremater ia lo reduce ddycurrent,
(c)using oftmagneticaterialoreduceoss rommagnetizationand emagnetizationnd
(d) singclosedoop esignor hecorenadditionoan rrangementof windingne oi l roundheothero mproveluxinkage.
UnderstandingheGeneration ndTransmissionfElectrici ty
Sourcesfenergyor
generationfelectricityreeither onrenewable
sourceshichre uclearowerndfossi luels r renewableourcessuch s hydropower,ind ower,so la rpower nd ene rgyrombiologicalrocesses.
27
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,i1i"""""""""""""""RfrPHICORGfrIIlSER3'|::::::::::::::::::::::::::::::::i:i:
r::: Name the rules n Box A, B and C. Complete he equations n box D and E
Renewable energ"ysources Nonrenewable energy sources
Power Tlansmission National Grid Svstem
38
ELECTROMAGNETISM
Analysing the Magnetic Effect of a Current-carrying Conductor
-€-_------- Northolei
CurrentI
Understanding the force on a current-carrying Conductor in a Magnetic Field
B MogneticT
field ,/ |
-Force Itl
Current
Analysing Electromagnetic Induction
field rr | |
\ |
Inducedurrent \l I____l
Analysing Tbansformer
Ideal transformer IV I
p _ |
\= l IV l = Ip
IV I I
n = 100 x7-!\ Vo= Vo I\ / l
Understanding the Generation and Thansmission of Electricity
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gHAPTER
ELECTRONICS
o fe
r
I
e
e rk l
@ UnderstandingheUses f the C.R.O.
1 A materialives ff hargedarticleswhen t is heated o a hightemperature.hisscalledhermionicemissionndhe articlesre alledthermions.
2 The hermionsmit tedncreaserapidly ith especto emperature.
3 A typicalhermionicpparatusastwospaced-outlectrodesnsidegas-filledlassube.
4 On emetal late erves sanodewhile nothertypicallytungstenfilamentra coatedilamentrelsea metalp latecoatedwi th acompoundf i t hasa separatefilament)ervesscathode.
5 Anelectricalupplys used or hefi lamenteatinghi le high .d.supply s put across he twoelectrodesopromotelectronlow.
6 A galvanometern series it h hecircuit easureshe urrentlow.
7 Byheat ingornot) he i lamentcoupledith hanginghepolarities
of he igh .d . crosshe lectrodes,experimentanbecarriedut oconfirmheemissionfelectrons.
8 Cathodeaysarebeams f fastmovinglectrons.
I Thepropertiesf cathodeayarestudiedhroughariousathodeaytubesC.R.T.)suchs he Maltesecrossube,hedeflectionubeandthePerrinube.
10 lt spropertiesnclude:
. lt movesna straightin e
. lt possessesegativeharge
. l t possessesomentumndenergy
. lt sdeflectedya magneticield
. lt is deflectedyanelectricieldan d
. lt producesluorescencehentstrikes uminescentcreen.
11 The tructurefa cathodeay scilloscopeC.R.O.)sshownnFigureelow.12 lt has hreemain arts:nelectronun, deflectionystemnd fluorescent
screen.13 Anelectronunconsistsfa filamentforheatinghecathode;cathodeto
produceathodeay eams);wire rid to educehe mountfelectronsoingthroughnd rightnessontrol)nd woanodesoneoaccelerateheelectronsand notheror ocus ontrol).
14 A deflectionystemonsistsf wosets fparallellateso controlheverticalandhorizontaleflectionsf hebeam.
15 The nner urfacef he ube oated ith in c ulphideormshe luorescentscreenwhichonvertsineticnergyo ight).
16 Lightsemittedy ha tmaterialt he nstanthat lectronsit t.17 Anoscilloscopesbasicallydevicehich isplaysgraphfanelectricalignal
and tshowsow ignalshangeve rime.18 Commonsesnclude easurementf voltages,easurementf shortim e
intervalsr requencynd isplayfwaveforms.
@ Understandingemiconductoriodes
1 Asemiconductorismaterialhoseonductivityies etweenhat fa metalndan nsulator.
2 ltsconductivitysaffectedy emperature,xposureo ight nd tscontentfimpurities.
3 The uter rbitsf he tomsfa materialndhe umberfelectronsnhabitingin he m eterminehe onductivityf hematerial.
4 The uter rbitsan edividednto nergyands:conductionand nd valenceband ith nenergyap eparatinghem.
5 Asemiconductoras ully ccupiedalenceand ith smallenergyapo heconductionandmakingta poor onductor.
6 But lectronsn he alenceand an cquireufficientnergyfromncreasentemperaturerexposureo ight)o ump crosshe ap omoven he onductionband nd onductlectricity.
7 Examplesfsemiconductorsncludeiliconnd ermanium,ach fwhich asfour lectronsn he uter rbit f he alenceand.
8 Asiliconrgermaniumto man harets our lectronsncovalentonds it htsneighborsormingregularrystalattice.
9 Electronsnhabitingn he alenceand re alledalencelectrons.10 Theireparturereatesolesunoccupiedpace)n he rystalattice.
T
coo.)o
(t,.)oo3
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n
p-
n
E
an O
n o
ts
P N
1 8
1 9
When he B -E orward ias sremoved,owillal l to ero.l. and . wil l ol low nd all o zerobecausef the everseias f theC- Bunction.
The ollectorurrentanhereforeeturned n or o f f byapply ingrremovinghe orwardias n heB-E erminalsakinghe ransistoro
behaveik e switcn.Figures od show pplicationfatransistors a currentmplifier,l i gh t on t ro l l edw i t ch , hea tcontro l ledwi tch nda soundcontrolledwitchespectively.
20
21
g O
ts
)
o .
a
@ AnalysingLogicGates
A ogicat esan lementaryuildingblock fdigitalircuits.It s anarrangementf electronicswitchesor he mplementationfBooleanogicalculations.Logicatesave ne utputnd neormorenputs.Everyerminalf a logic ate salwaysn oneof the wobinaryconditions:ow 0or alse)rhigh1or rue),epresentedya ow ndhigh oltageespectively.Anassemblyf he ariousogic atecomb ina t i ons nab les the
67
implementationsf complexogic perationseededor heconstructionfcomputersnd ther lectronicystems,Therere ive asicogic ates:AND,R,NOT, ANDndNCR.Theirymbolsnd ruthablesre hownnFigure oe.
lnDUt::AnPnt..,gutput0 0 00 4
I 01 n
U 01
1 1AND gote
A--f---__\I F X
B-l____J
A Input.',.Butput0 0 00 1 1
1 n 4
I
1 1 1ORgote
NAND oote
NO T gote
NOR gote
91 0
Combinot ionof two
logic gotes
A
B
11
12
13
1 4
r,pul4,:,..
ln.Fut':,:,1:':',"fi,ttt,,',',,
0utput,:,],:,,,,,X],,,,:,
0 0 1
0 4I 1
1 0 11 1 0
lnpul. . . .4 ' l , '
Influt.:,1..,...Ell.,,,.
oUtpul.X
n 0,l
I
n 1 01 0 0
1 1 0
A--J---lI p-x
s--I___J
Logicatesan e ombinedor he urposefproducingore omplexunctionsor or he ubstitutionfone ype fgateoranother.Truthablesre ften sedinsteps)owork ut he unctionfacombinationfgates.Figureelowhows simplexamplef he ombinationf wo ogic ates.
tn:put'a ,,lnput
'B G.,Ontgut,Xi . ,=C 'A
0 0 1 00 1 0 01 0 1 1
1 1 0 0
Some pplicationsf ogic atesncontrolystemsncludeafetyystem,treet
lightingsnd ecurityystem.Anexamplefa 2-inputs NDcircuit anbeone hatwould urnon he ireextin-guisherhe n ot hheheat etectornd he mokeensornputsre riggeredsimultaneously.Streetightingsre urnednbya 2-inputsRgate,he nputsfwhich reasignalro m ime lock nd signalrom daylightensor.AcombinationfoneNOT nd wo ND atesora simpleual-switchecuritysystem hownnFigureelow,hich ouldnlockhe oor hen oth witchesare norsound nalarmf hehiddenwitchsno t urnedn.
Switch
B
Switch
(o hiddenswitch)
fi B c ..,:OutpUt...X '. . ,'B
,,,Outpttt..V.,*,At',,B
0 0 1 0 00 I 0 0 0
Only witch son 1 0 1 0 1Both witchesreon 1 1 0 1 l 0
ON ON
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gHAPTER
KADIOACTIVITY
m UnderstandingheNucleus f an Atom
1 An atoms thesmallestni t f a
chemicallementha thas tsownchemicalroperties.
2 Atoms remade pof fhreemajor
types fsubatomicarticles:roton,
neutronnd lectron.3 Protonsndneutrons,o th re
known s nucleons,ake p hedense, assivetomicucleusn hecentre hile lectronsorm cloud
orbitingrroundhenucleus.4 Electrons ave negativeharge
and re heeast assivef he hree.5 Protons ave positiveharge nd
are bout 836imes oremassivethan lectronshile eutrons,hichhave mass qualo heprotons,
carry ocharge.6. Everyorm f arrangementf the
subatomicart ic lesn an atom scal lednucl ide.
7 Nuclidesfdifferentlementsiffer
in thenumber f thesubatomicparticleshey ontain,articularlyhenumberfprotons.
8 Nuclidesf hesame lementls oexistnmorehan ne orm.
9 They ave hesame umber fprotonsutdiffern thenumberfneutrons.
10 Nuclidesf thesame lement ithdi f ferentumbersf neutronrecalledsotopes.
11 A notation,alledhe tomicymbol,
isdevisedodistinguishne sotopefrom nother.12 Thenumberf protonsnanatom,
A, scalledheatomic umberorprotonumber).
13 The otal umberf profonsndneutronsnanatom, , scalledhenucleonumberormass umber).
14 Hence,henuclidefanelementis epresentedylX .
15 For xample,!ti
andI i
ar e sotopesf heelementithiumLi ):1;
has
protonsnd (=6-3)eutronshile]1 ;ha s protonsnd (=7-3)eutrons.
sp| Analysing adioactive ecay
1 Radioactivityr adioactiveecaysanaturalnd pontaneousrocessywhich
theunstabletoms f anelementisintegratendemit nergeticarticlesrphotonsn he orm f onizingadiations.
2 Such missionouldither ak ehe toms ore tabletastate f owernergy(whileetainingheoriginalorm) r changehenucleusompletelynd husproducedifferentlement.
3 Whenhe ater appens,hedecayingucleusscalledheparentucleusnd
the esultantscalledhedaughterucleus.
4 The mittedarticlesnd he aughterucleusre nownsdecayroducts.5 Threeommonadioactiveecaysrealpha ecay, eta ecay ndgamma
emission.6 Alpha ecaysaprocessnwhich particleithwo eutronsnd wo rotonss
ejectedromhenucleus.7 The articles denticalo henucleusfa heliumto m8 Beta ecaysa processnwhich nelectronsemittedromhenucleus.
I Duringheprocessfemittinglpha rbeta articlehenucleusls oossests
excessnergyyemittingulsesfelectromagneticadiationnd he rocesss
cal ledammamission.10 ExamplesfalphaecayRadium-226)nd eta ecaylodine-131)nd amma
emissionRadium-214)rittenn ormulare s ollowsespectively:
'i2i$,Rr,.+rioq.R*..+..1..tt;,6|:t',.,,,.,t;,!;':,;,'t,. ' ' ' '
..lltll'.1,..'''..*.llfl|'L,,,:",',;,;*"r!';ei""';',:"""L"""'2$Bi+'#Pu-1C;:t
11 The haracteristicsf adioactivemissionsre ummarizedelow.
ChaiacteiiiticS Alphadecay Beta ecay Garn,nrarnisCion
ParticleCharge) Helium+vs1 Electron-ve) Photonno harge)
Symbol !He r cr .feor !B I
Approximateass 4 proton
MASSES-k proton assI o Jo
Nit
lonising ffect Strong Weak Veryweak
Penetratingower 7 cm nair 3mm naluminum 15 m n ead
Shielding aterial Paper,kin,clothes
Plastic,lass,ightmetals
Dense etal,
concrete,arth
Effect f amagneticield
Small eflection Large eflection Noeffect
Speed l l ^ t ^ l -" y ' " 1 0speedf ight
Up of i speedfl igh t
Speedf ight
<)
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12
1 3
Commonetectorssedor hedetectionf adioactivityncludeparksounter,Geiger-Mullerube, loudhambers,old-leaflectroscope,cintillationetector(sodiumodide)nd hotographiclates/films.
Figurebelowhowshe chematicfa Geiger-Mullerube ndFigureshowsthe racksf he hreeypes f adiationnacloud hamber.
+
45 0V
Aluminumubecothode
Centrewire
onode
i { ^
S
f
I
I
I
CX,
Thick ndstroight
- \ l) /-+\l)t/
i \//J\ \
J /
(D
BThin nd r regu lo r
b
\ \ \ t , l / t
"\ \ r \ ,
' l ' , ,\ r t l t l l
\ \ , / . '\ \ \ ' /
(D
vI
Shortond scottered
14 Theate f adioactivityecaysunaffectedy he hemicalhangertemperature.15 However,heactivityr heaverageumberfdisintegrationer econdn a
radioactiveecaysalwaysroportionalo he umberf he emaininguclei.16 The alf-lifefa radioactiveaterialanbedefineds he ime equiredor he
materialodecayohalf f ts nitialalue.17 The alf-livesfsomeadioactiveaterialsre x 108 earsorUranium-235,
1620 earsorRadium226, 5hoursorSodium24,52econdsorRadon-220and x 10-7econdsorPolonium-212.
18 Carbon-datingsanapplicationf hehaltlife ropertyf adioactiveaterials.
sf,l Understandinghe Uses f Radioisotopes
lsotopesre uclideshich av ehe ame tomicumberutdifferintheas snumber.Radioisotopesre adioactivesotopes.Someadioisotopesccur atural lyuch slH,
3:U,l !Raand!iRb.Someadioisotopesre rtificiallyroducedyneutronctivation,issionroductseparationrchargedarticleombardment.Examplesfartificiallyroducedadioisotopesre}iio,iiMn,11Nand lll.
The ollowingshow ome f he pplicat ionsf adioisotopesn he ariousields:
234
56
Thinmico .Argongo sot low pressure
Arsaof Application Ra.di6iSol0p,gs AppliCafione
Medicine lodine-131Cobalf60
It .
2.1. usedo reathyroidisorders2. sterilizeurgicalnstruments
Agriculture 1. Phosohorus-322. Selenium-75
1. moleculariologynd eneticsesearch2. proteintudiesn ife cienceesearch
Archaeology 1. Carbon-14 1. datingfarchaeologicalrtifact
lndustry Cesium-137
Throium-230
1 .
2.
1. omeasurehe iquidlownoilpipelines
2. Providesluorescencencoloredlazes
53
@ UnderstandingNuclearEnergy
1 Atomicmassuni t . r a.m.u. ,s
definedobe* of hemass fon eatom f sotop5arbon-1,It is a unitoften sed o express
atomicndmolecularasses.
Themass fcarbon-12s 1.99310'6kgand herefore
i a.m.u.;r'1.661g+r:1n.
Radioactiveecayesultsna ossofmass, hichsconvertedoenergy
accordingo theEinsteinormulaE=mCwhere s energyn oules,
m smassnkilogramsnd is he
square f t hespeed f i gh t nvacuumnms-1= 3x 108ms- l2 .When nucleusissions,tsplitsnto
two rmore malleruclei.In he rocess,wo r hree eutronsarealso mittednd hesum f hemassesf he ragmentss esshanthe riginal ass.About .1Yo f heoriginalassslostandconvertedntoenergyaccordingoEinstein'squation,SinceC in the ormulas relativelylargenvalue, bigamount fenergycanbeobtainedromafractionf hemater ia lhroughheprocessf
nuclearission.A nuclearhaineactionefersoaprocessnwhich eutronseleasedin f iss ion roducen addi t ionalfissionnat east neurtherucleus.Th isnuc leusn tu rnp roduces
neutronsnd heprocessepeats,The rocess ay econtrolleds nnuclearowereactorruncontrolledas nnuciearombs.Figurehowssimplifiediagramfa nuclear eactor here hainreac t i on f nuc lea riss ions
control ledo generatelectr icalenergy.Uranium-235s used s uelandgraphiclocks ith avitieservesthemoderatorcontro lods) ocontrolheneutrons.
10
11
12
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1 4
1 5
Carbonioxidercold ater cts s
coolanto ransferheheat ut o urn
thegenerator.
Shortagef energyources often
usedo ustifyor heuse fnuclearpower hileisks faccidenthich
will eado ossnhumanives nd
contaminationf environmentre
considerationssed gainstuclearreactor.
Control od drive
Ho tcoolqntto heotexcnongers
Coolont
Cool coolont from heot exchongers
Nuclearusions heprocessywhichmultipleucleiombinefter
col l idingt high peedo form
heavierucleus.Itonly ccursn h eextremelyigh-
energynd emperatureonditions.Nuclearus ion f ight lementsreleasesnergyuch s he rocess
which owershe un ndhe tars.Hydrogenomb xplosionscausedby fus ionof Hydrogen-2ndHydrogen-3ntoHelium-4.
All adioactiveaterialsus there-
fore eclearlyabeledndprecau-
tions uc h swarningigns,ppro-priateui ldingnd ts ocal i tynd
properontainerocontainhema-
terials.Specialehicles,hieldingnd ro-
tectiveears ust eprovidedopro-
tect heenvironmentswell s hepeopleandlinghe ubstance.
lf notmanagedroperly,adioactive
materialsan ontaminateheenvi-
ronmentora on gime nd et nt o
ou rood hain hich illea doseri-
ous icknessesuch seye ataract,
cancernd ellmutation.
Radioactiveastesormallylassi-
f ied s ow-level,edium-levelr
high-levelastes,ccordingo he
amountnd ypes f adioactivityn
them.Three eneralr inciplesreem-ployedn hemanagementf adio-
active astes:(i ) concentrate-and-contain:
thewastesconcentratednd
thensolated:(ii) di lute-and-disperse:
th ewastes dilutedo accepf
ableevelsndhen ischarged
to he nvironment,nd(i i i) elay-and-decay:
thewastesstoredndts adio-activitys allowedo decrease
naturally.Low-levelastesgeneratedrom
hospitals,aboratories,ndustry,nd
the uclearuel ycle.
8 ltcomprisesaper,ags,ools,loth-
ing, i l ters ndetc.which ontain
small mountsfmostlyhort-lived
radioactivity.
9 l t is notdangerouso handle,ut
must edisposedfbyburialnshal-
lo wandfi l li tes.
10 lt s often ompactedr ncinerated
in a closedncineratorefore is -posal.
11 lntermediate-levelaste ontains
higher mountsf radioactivitynd
requirespecialhieldingnhandling.
12 lt ypicallyomprisesesins,hemr-'
ca l ludge,eactoromponentsnd
contaminatedaterialsromeactor
decommissioning.13 lt may esolidifiednconcreterbi-
tumenordisposal.
Generallyhort-livedastemainly
fromeactors)sburied,utong-livedwaste from eprocessinguclear
fuel) il l edisposedfdeep nder-ground.
High-levelastemay e he pent
fuel tself r heprincipalasterom
reprocessinghe uelmaterials.
Itcontainshehighly-radioactiveis-
sion roductsnd ome eavy le-
ments ithong-livedadioactivity,7.
Itgeneratesconsiderablemountf
heat nd equiresoolingswell s
specialhieldinguringandl ingndtransport.Th ewaste houldesealednside
speciallassnd tainlessteelcan-
istersoreventualisposaleep n-
derground.
1 6
1 4
1 5
1 6
1 7
1 8
1 9
sf| ProperManagementof RadioactiveSubstances
1 Radioactiveaterialsamagerde-stroyiving ells nd hereforerehazardousohumaneinq.
1 7
54