GENERALPHYSICS2 ChargePolarization
Onestep(first)ofchargingbyinduction.
Lesson1:ElectricForcesandFields ex.chargedcombattractsanunchargedpieceofpaper(whichisan
insulatorsonoelectronswillflowthroughit)
ElectricCharge
Fundamentalpropertyofmatter. Coulomb’sLaw
Describesthe“electric-ness”ofparticles. Anelectricchargeexertsaforceofattractionorrepulsiononotherelectric
charges.
TypesofCharges
Kq q
BenjaminFranklinstatedthattherearetwocharges,positiveandnegative. F = r12 2
Likechargesrepel,unlikechargesattract. k=9.0x109 Nm2 /C2 (Coulombconstant)
ElementaryCharge ElectricField
e=1.60x1019Coulomb
IsavectorandisdenotedbyE .
Ifpositive(proton),itisradiallyoutward.
ParticleCharges Ifnegative(electron),itisradiallyinward.
Proton +e=+1.60x1019 C
Electron -e=-1.60x1019 C
Neutron nocharge
PropertiesofElectricCharge
1.Chargecomesinquantizedunits.
Chargecomesinmultiplesofe(...,-2e,-1e,0e,+1e,+2e,…)
Quarks
Mattercontainsatoms.
(a)isadipole;(c)isnot,-ehaslesselectricfieldlinesthan+e.
Atomscontainelectronsandanucleus.
Anatom’snucleuscontainsprotonsandneutrons.
ElectricFieldLine
Protonsandneutronscontainquarks.
Setofcontinuouslinesthatarealwaysparalleltotheelectricfield.
Theyarenotreal.
TypesofQuarks
Top (⅔)e Bottom (-⅓)e
Notes
Charm (⅔)e Strange (-⅓)e
1. Mustbeginona“positive”chargeandendona“negative”charge.
Up (⅔)e Down (-⅓)e
2. Magnitudeofanelectricfieldisthelargestforthefieldoflines
thataremostcloselyspacednearthecharges.
Protonscontain2Uand1D.
3. Neverintersecteachother.
Neutronscontain1Uand2D.
Thepresenceofachargeproducesanelectricfield.
2.Chargeisconserved.
Electricfieldisrelatedtotheelectricforce.
LawofConservation
Chargecanmovefromplacetoplace,andfromoneobjecttoanother, F = ∣q ∣ E → E = ∣Fq∣
K ∣Q∣
butthetotalchargeoftheuniversedoesnotchange. E = r2 Units:NewtonperCoulomb(N/C)
Electronsaretheonebeingtransferred,notprotons,becausetheyare
notattachedintheatom’snucleus.
TypesofCharging
1.ChargingbyContact
Transferofachargefromonematerialtoanotherbyphysicalcontact
betweenmaterials.
Howtomakeanobjectpositively-charged?Moveapositively-charged
objectsuchasglass(whichisusuallypositive,whilerubberorplasticis
usuallynegative).Thenegativechargesfromtheobjectwillbe
transferredtotheglass.
2.ChargingbyInduction
Processofgivingoneobjectanetelectricchargewithouttouchingthe
objecttoasecondchargedobject.
Forexample,thisisdonewhenanegatively-chargedobjectismoved
nearanotherobject,polarizingit.Theelectronsmoveawayintoa
groundingpathorwire,whichmakestheobjectpositively-charged.
,
Lesson2:ElectricPotential EquipotentialLinesandSurfaces
Anequipotentialsurfaceisa3DsurfaceonwhichtheelectricpotentialVis
Battery thesameateverypoint.
Thepositivesideiscalledpositivepotential,negativesideisnegative Electricfieldlinesandequipotentialsurfacesarealwaysperpendicular.
potential.
ElectricPotentialEnergy BOOK
Whenachargedparticlemovesinanelectricfield,thefieldexertsaforce
thatcandoworkontheparticle.TheworkisthePEelec Capacitance
Sinceelectricforceisconservative,similartothegravitationalforce,then
ΔP E elec = − W = − F elec Δx
ΔP E elec = − q EΔx
Iftwochargesareinitiallyseparatedbyadistancer 1 ,thenbrought
togethertoafinalseparationr 2 ,then
kq q kq q
ΔP E elec = P E elec2 − P E elec1 = r12 2 − r11 2
Butisr 1 isininfinite(q1 andq2 areinfinitelyapart),then
kq q
P E elec = r1 2
Ifwehaveacollectionofpointcharges,thetotalPEelec isthesumofthe
potentialenergiesofeachpairofcharges.
kq q kq q
ΔP E elec = P E elec2 − P E elec1 = r01 1 − r02 2
ElectricPotential
Scalar.
Oftenreferredtoassimplythe“potential”.
ΔP E kqQ kQ 1 Q
V = q elec = 1q r = r = 4πε r
0
Unit: Volt(V)
V=J/CorNm/C
1eV=1.60x10-19 J
ε0
Permittivityoffreespace,aconstant.
Howanelectricfieldpropagatesormovesinemptyspaceoravacuum.
ElectricPotentialandE lectricField
Magnitudeanddirectionofelectricfieldarerelatedtohowtheelectric
potentialchangeswithposition.
EisproportionaltotherateofchangeofVwithposition.
PotentialDifferenceorV oltage
Scalar.
ΔP E elec = − W = − q EΔx
ΔP E
ΔV = q elec = − E Δx
Negativesign(-)indicatesthattheelectricfieldgoesfromaregionof
highpotentialtoaregionoflowpotential.
DuetoaPointCharge
kq
V = r
DuetoaCollectionofCharges
V =V1+V2+V3
kq kq kq
V = r11 + r22 + r33
DuetoChargedConductingSphere
kq
Outside V = r
kq
Inside V = R