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Physics Notes Electromagnetism Davesim

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    Electricity ElectromagnetismInGravitation,we learnt that amass (A) gives rise to a gravitational field

    around it. Another mass (B) in this field will experienced an attractive

    gravitational forcebymass (A). InElectricField,we learnt thatacharge (A)

    gives rise to an electric field. Another charge (B) in this field will either

    experience an attractive or repulsive force by charge (A). In

    ELECTROMAGNETISM, we will learnt that a moving charge constitute to

    current. Besides electric field, the current gives rise to a magnetic field

    around it.Wewillalsodiscusshowamagnetic forcecanbecreated in the

    presenceofcurrentandmagneticfield.

    Dave Sim @

    Raffles Institution

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    IN TRODUCTIO N

    MAGNETICFIELD

    The number of lines per unit crosssectional area is

    proportionalto themagnitudeofB. Ifthe field isuniform, the

    fieldlinesareevenlyspaced.

    Werepresentthemagnitudeanddirectionofamagneticfield

    by themagnetic flux density B. (analogous to electric field

    strength,E inelectricfieldandgravitationalfieldstrength,g in

    gravitationalfield.)

    ItsunitistheTesla(T).

    s in

    s in

    =

    =

    B

    B

    F B I LF

    BIL

    Amagnetic field is defined as the region in space in

    whichamagnetwillexperienceamagnetic forcewhen

    placedatthatpoint.

    The direction of themagnetic field is the direction in

    whicha smallmagneticnorthpolewillmove ifplaced

    there.

    ThemagneticfluxdensityBatapointinamagneticfield

    is the forceperunit length thatactsonawirecarrying

    unitcurrent,lyingatrightanglestothemagneticfield.

    N

    S

    (a)Barmagnet (b) Ushapedmagnet

    Fieldlines

    closetogether

    Blarge

    Direction

    ofBatP

    B

    small

    Parallelfield

    linesBisconstant,i.e.a

    uniformfield

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    C O NC EPT 1 - M A G NETIC FIELD DUE TO C URRENT- C A RRYING C O NDUC TO R

    CASE1 MAGNETIC FLUX DENSITYDUE TOAN INFINITELYLONG STRAIGHT WIRE

    CASE2 MAGNETIC FLUX DENSITYDUE SOLENOID

    Aconductorcarryinganelectriccurrentalsosetsupamagnetic

    field.

    where B=fluxdenstiy

    I=currentinthewire

    r=perpendiculardistanceofPfromwire

    0 = a constant of proportionality known as the

    permeabilityoffreespace( 7 14 10 Hm ).

    Current flowing through a solenoid (L >> d) also sets up a

    magneticfield.

    n=numberofturnsperunitlengthof solenoid,N/L

    ateitherendofthesolenoid,B=(nI)

    2

    = o

    IB

    r

    I

    r

    P

    0= B n I

    currentflowingintopaper

    currentflowingoutofpaper

    current flowing

    out of paper

    Fig. 10

    current flowing

    into paper

    B

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    CASE3 MAGNETICFLUX DENSITYDUECIRCULARCOIL

    Current flowing through a circular coil (L

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    CONC EPT 2 - M A G NETIC FO RC E O N A C URRENT- C A RRYING CO NDUCTO R IN A M A G NETIC FIELD

    ACURRENTCARRYINGCONDUCTOR INAMAGNETIC FIELDEXPERIENCESAFORCE.

    DIRECTION OFMAGNETICFORCE

    MAGNITUDE OF MAGNETIC FORCE Themagnitudeof the forceFonawire inamagnetic field is

    directlyproportionalto

    1) thecurrentIinthewire

    2) thelengthLofthewireinthefield

    3) themagneticfluxdensity,B

    4) theanglebetweenthecurrentand themagnetic flux

    density,B,whenbothareinthesamedirection.

    1) Magneticforceismaxwhen is =902) Righthandgrip pleasenotethatforceisIXB,whereI

    andBareinthesamedirection.

    ( ) ( )sinmagnetic

    F L IXB B I L = =

    sin=B

    F BIL

    I

    B

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    A PPLIC A TIO NS OF CO NC EPTS

    CASE1: FORCESBETWEEN TWOPARALLELCURRENTCARRYINGCONDUCTORS

    Case1:LikeCurrentattracts Case2:Unlike Current repels

    Note:MagnitudeofFB

    Theampereisthatsteadycurrentwhich,whenitisflowingineachoftwoinfinitelylong,straight,parallelconductorswhichhave

    negligibleareasofcrosssectionandare1metreapartinavacuum,causeseachconductortoexertaforceof2107Noneach

    metreofthewire.

    X Y

    I1 I2

    r

    X Y

    I1 I2

    r

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    B

    Three longverticalwirespass through the cornersofan

    equilateraltrianglePQR.PandRcarriescurrentdirected

    into theplaneof thepaperandwireQcarriesacurrent

    directed out of the paper. All three currents have the

    samemagnitude.Whicharrowshowsthedirectionofthe

    resultantforceactingonP?

    B=oI/2r.6.0104T6.7105T3.2103Ntowardsthe

    wire.

    ThefigureontherightshowsalongwireXYcarryinga

    currentof 30A. The rectangular loopABCD carries a

    currentof20A.Given:a=1.0cm,b=8.0cmandL=30cm.

    (a) Calculate themagnetic fielddue to the current

    inXYalong

    (i) AD

    (ii) BC

    (b) Calculatetheresultantforceactingontheloop.

    B

    Three long wires W1, W2 and W3 carrying the same

    current I are arranged in the configuration as shown

    below.What isthedirectionoftheresultantforceacting

    onW1?

    A Totheright

    B Totheleft

    C Downwards

    D Upwards

    P

    RQ

    A

    B

    C

    D

    E

    I

    a

    aa

    W3

    W2W1

    D

    C

    20A30A

    Y

    X A B

    L

    a b

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    CASE2: TORQUEON ACURRENTCARRYINGCOIL IN A MAGNETICFIELD

    MagnitudeofFB

    Case1: =0 i.e.whentheplaneofthecoilisparalleltoB. Case2: =90,i.e.whentheplaneofthecoilisperpendicular

    toB

    I

    P

    S

    Q

    I

    R

    Y

    B

    (a) SIDEVIEW

    current

    out

    b

    (b) TOP

    B

    P

    current

    down

    Q

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    CONC EPT 3 MAGNETIC FORCE ON A CHARGED PARTICLE IN A MAGNETIC FIELD

    MAGNITUDEOF MAGNETICFORCE

    Considerachargedparticlemovinginauniformmagneticfield

    withvelocityv.

    Note:

    1) Note the sign of the charge when determining the

    directionofFB

    2) Thepath travelled isa circularpathas themagnetic

    forcewhichisalwaysperpendiculartothedirectionof

    motionprovidesthecentripetalacceleration.

    Case1:PostiveCharge

    Case2:NegativeCharge

    72.8 10 Hz

    Anelectronofchargeeandmassmdescribesacircularpathofradiusrwhenitisprojectedwithvelocityvinto

    auniformmagneticfieldoffluxdensityB. Showthatthefrequencyofrevolutionisgivenby2

    =Be

    fm.

    Howmanyorbitspersecondaremadebyanelectronifthefluxdensityis1.0103T?

    (e=1.61019C;m=9.110

    31kg.)

    sinB

    F Bqv =

    Fm=BQv

    v

    v

    M

    FB

    v

    N

    FB

    sin

    sin

    sin

    B

    B

    B

    F BIL

    dqF B L

    dt

    F Bqv

    =

    =

    =

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    2.6107ms

    1

    1.1107s

    2.21012J

    7.0

    10

    6V

    An particle, ofmass 6.7 1027 kg and charge +2e ,was injected at right angles into a uniform

    magneticfieldoffluxdensityB=1.2T.Ittravelsinacircularpathofradius 0.45m.Calculate

    (a) itsspeed,

    (b) itsperiodofrevolution,

    (c) itskineticenergy,and

    (d) thepotentialdifferencethroughwhichitwouldhavetobeacceleratedtoachievethisenergy.

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    Undeflected

    Undeflected

    Upwards

    undeflected

    Thefigureshowsaparticle,ofcharge+qandmassm,enteringauniformmagneticfieldBthatisdirected

    downwards into theplaneof thepaper.Theparticle is travellingwithvelocityvatrightangles to the

    field.

    Auniformelectric field isapplied in thesame regionas themagnetic field so that theparticlepasses

    throughundeflected.

    (a) WithanarrowlabelledE,thedirectionoftheelectricfield.

    (b) Stateandexplaintheeffect,ifany,onaparticleenteringtheregionofthefieldsiftheparticlehas

    (i) chargeq,massmandspeedv,

    (ii) charge+q,mass2mandspeedv,

    (iii) charge+q,massmandspeed2v,

    (iv) nocharge(i.e.particleisneutral),massmandspeed2v.

    X X X X

    X X X X

    X X X X

    X X X X

    X X X X

    particle

    region of uniform

    magnetic field into

    planeofpaper


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