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Chapter27 Student

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    Chapter 27. Current andChapter 27. Current and

    ResistanceResistanceA PowerPoint Presentation byA PowerPoint Presentation by

    Paul E. Tippens, Professor ofPaul E. Tippens, Professor ofPhysicsPhysics

    Southern Polytechnic StateSouthern Polytechnic State

    UniersityUniersity

    !2""7

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    #b$ecties%#b$ecties% After co&pletin'After co&pletin'this &odule, you should bethis &odule, you should be

    able to%able to%( )e*ne)e*ne electric currentelectric currentandand

    electro&otie forceelectro&otie force..

    ( +rite and apply+rite and apply #h&s law#h&s lawto circuitsto circuitscontainin' resistance and e&f.containin' resistance and e&f.

    ( )e*ne)e*ne resistiityresistiity of a &aterial andof a &aterial and

    apply for&ulas for its calculation.apply for&ulas for its calculation.

    ( )e*ne and apply the concept of)e*ne and apply the concept of

    te&perature coe-cient of resistancete&perature coe-cient of resistance..

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    Electric CurrentElectric Current

    Electric currentElectric current is theis the

    rate of the /ow of char'erate of the /ow of char'e

    00throu'h a cross1sectionthrou'h a cross1section

    AA in a unit of ti&ein a unit of ti&e tt..

    QI

    t=

    QI

    t=

    1C1 A

    1 s=

    1C1 A

    1 s=

    #ne#ne a&perea&

    pereAAis char'e /owin'is char'e /owin'

    at the rate of oneat the rate of one coulo&b percoulo&b per

    secondsecond..

    AA

    11+ire+ire

    00

    tt

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    E3a&ple 4.E3a

    &ple 4.The electric current inThe electric current ina wire is 5 A. 6ow &any electronsa wire is 5 A. 6ow &any electrons/ow past a 'ien point in a ti&e of/ow past a 'ien point in a ti&e of s8 s8

    9 5 A 9 5 A

    ;q

    I q It

    t

    = =

    ;q

    I q Itt

    = =

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    Conentional CurrentConentional Current

    &a'ine a char'ed capacitor with&a'ine a char'ed capacitor with Q = CVQ = CVthat is allowed tothat is allowed to

    dischar'e.dischar'e.Electron /ow%Electron /ow%TheThe

    direction of edirection of e11 /owin'/owin'

    fro& : to .fro& : to .Conentional current%Conentional current%The &otion of ;The &otion of ;

    fro& to : has sa&efro& to : has sa&e

    e.

    11

    1

    Electron/ow

    1 1

    e1

    Conentional/ow

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    CurrentCurrent

    The number of charges that pass through the area in timeThe number of charges that pass through the area in timettN = n(|N = n(|vv||t)(|A|)t)(|A|)

    The total charge that passes through is q times this numberThe total charge that passes through is q times this number

    q = qnq = qnvv AAtt

    The current I =The current I =q/q/ tt

    Current , I = qnCurrent , I = qn v Av A

    Current Density , J = I /A = qnCurrent Density , J = I /A = qn vv

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    Current DensityCurrent Density

    The current density (associated with one type of chargeThe current density (associated with one type of charge

    carriers) is defined as a product of the drift velocity, thecarriers) is defined as a product of the drift velocity, the

    concentration of charge carriers and the charge of the carriers:concentration of charge carriers and the charge of the carriers:

    J

    J vd

    =nq

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    Electric Current in a ConductorElectric Current in a Conductor

    In a conductor, current density is proportional to the electricIn a conductor, current density is proportional to the electricfield vectorfield vector

    J E= (h!"s law)(h!"s law)

    The constant of proportionalityThe constant of proportionality is called the conductivityis called the conductivityof the conductor.of the conductor.

    #nder a steady flow of charged particles#nder a steady flow of charged particles

    along a conductor, the current across anyalong a conductor, the current across any

    cross section of the conductor has thecross section of the conductor has thesa!e value$sa!e value$

    II

    II

    II

    %e assign this value to the current in the%e assign this value to the current in the

    conductor$conductor$

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    Electro&otie BorceElectro&otie Borce

    AA source of electro&otie force =e&f>source of electro&otie force =e&f>is a deice that uses che&ical,is a deice that uses che&ical,

    &echanical or other ener'y to proide&echanical or other ener'y to proide

    the potential di

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    +ater Analo'y to EDB+ater Analo'y to EDB

    &ow

    pressure

    Pump%ater

    'igh

    pressure

    alve%ater

    low

    Constriction

    Source ofEDB

    Resistor

    'igh

    potential

    &ow

    potential

    *witch

    E

    RI

    1

    TheThe source of e&fsource of e&f=pu&p> proides the=pu&p> proides the

    olta'eolta'e=pressure> to force=pressure> to force electronselectrons=water> throu'h electric=water> throu'h electric resistanceresistance

    =narrow constriction>.=narrow constriction>.

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    Electrical Circuit Sy&bolsElectrical Circuit Sy&bols

    Electrical circuitsElectrical circuitsoften contain one oroften contain one or

    &ore resistors 'rouped to'ether and&ore resistors 'rouped to'ether and

    attached to an ener'y source, such asattached to an ener'y source, such as

    a battery.a battery.The followin' sy&bols are oftenThe followin' sy&bols are often

    used%used%

    + - + -- + - + -

    +round attery-+

    -esistor

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    Electric ResistanceElectric Resistance

    Suppose we apply a constant potentialSuppose we apply a constant potentialdi

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    #h&s Gaw#h&s Gaw

    #h&s law#h&s lawstates that the currentstates that the current throu'h a 'ien conductor is directlythrou'h a 'ien conductor is directly

    proportional to the potential di

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    E3a&ple 2.E3a&ple 2. +hen a+hen a 1@1@battery isbattery is

    connected to a li'ht, a current ofconnected to a li'ht, a current of 55&A&Ais obsered. +hat is theis obsered. +hat is theresistance of the li'ht *la&ent8resistance of the li'ht *la&ent8

    Source ofEDB

    R

    I

    1

    V = 3 @

    5 &A

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    A&&eterA&&eter@olt&eter@olt&eter RheostatRheostatSourceSource

    of EDBof EDB

    -heostat

    A

    Gaboratory Circuit Sy&bolsGaboratory Circuit Sy&bols

    @ .!f

    -

    +

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    Bactors A

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    Bactors A

    . The. The te&perature Tte&perature Tof the &aterial.of the &aterial.The hi'her te&peratures usuallyThe hi'her te&peratures usually

    result inresult in hi'herhi'herresistances.resistances.

    . The Hind of. The Hind of &aterial&aterial. ron has &ore. ron has &ore

    electrical resistance than aelectrical resistance than a

    'eo&etrically si&ilar copper'eo&etrically si&ilar copperconductor.conductor.

    RRoo R I RR I R

    oo

    RRiiI RI RccCopperCopper ronron

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    Resistiity of a DaterialResistiity of a Daterial

    TheThe resistivityresistivity is a property of ais a property of a&aterial that deter&ines its electrical&aterial that deter&ines its electrical

    resistanceresistance RR..Recallin' thatRecallin' that RRis directlyis directly

    proportional to len'thproportional to len'th LLandandinersely proportional to areainersely proportional to areaAA,,

    we &ay write%we &ay write%

    or

    L RA

    R A L = = or

    L RA

    R A L = =

    The unit of resistiity is theThe unit of resistiity is the oh&1&eteroh&1&eter

    ==

    &>

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    E3a&ple .E3a&ple .+hat+hat len'thlen'thLLof copper wireof copper wire

    is re;uired to produce ais re;uired to produce a & & resistor8resistor8Assu&e the dia&eter of the wire isAssu&e the dia&eter of the wire is 44

    &&&& and that the resistiityand that the resistiity of copper isof copper is4.72 3 4"4.72 3 4"1J1J ..&&..

    LR

    A=

    LR

    A=

    Re;uired len'th is%Re;uired len'th is%

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    Te&perature Coe-cientTe&perature Coe-cient

    Bor &ost &aterials, the resistanceBor &ost &aterials, the resistance RRchan'es in proportion to the initialchan'es in proportion to the initial

    resistanceresistance Roand to the chan'e inand to the chan'e in

    te&peraturete&perature tt..

    /R R t = /R R t = Chan'e inChan'e in

    resistance%resistance%

    TheThe te&perature coe-cient ofte&perature coe-cient of

    resistance,resistance, is the chan'e in resistanceis the chan'e in resistance

    per unit resistance per unit de'reeper unit resistance per unit de'reechan'e of te&perature.chan'e of te&perature.

    /

    /

    1; #nits:

    C

    R

    R t

    =

    /

    /

    1; #nits:

    C

    R

    R t

    =

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    E3a&ple .E3a&ple . The resistance of a copperThe resistance of a copperwire iswire is ."" &."" &atat 2"2"""CC. +hat will be its. +hat will be its

    resistance if heated toresistance if heated to J"J"""CC8 Assu&e8 Assu&ethatthat 9 "."" ?C9 "."" ?Coo..

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    ConductiityConductiity

    AA ConductiityConductiity &easures of a&aterialKs ability to conduct anelectric current

    1 1 or

    = =

    1 1 or

    = =

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    Electric PowerElectric Power

    Electric powerElectric powerPP is the rate at whichis the rate at whichelectric ener'y is e3pended, or worH perelectric ener'y is e3pended, or worH per

    unit of ti&e.unit of ti&e.

    V q

    V

    To char'e C% +orH 9To char'e C% +orH 9

    ;@;@ and

    or! qV q" I

    t t t= = =

    SubstituteSubstitute q = It ,q = It ,

    then%then%VIt"

    t= P = VI

    I

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    Calculatin' PowerCalculatin' Power

    Usin' #h&s law, we can *nd electricUsin' #h&s law, we can *nd electric

    powerpowerfro& any two of the followin'fro& any two of the followin'

    para&eters%para&eters% currentcurrent II,, olta'eolta'eVV, and, andresistanceresistanceRR..#h&s law%#h&s law% V = IRV = IR

    0

    0; ; V" VI " I R "R

    = = =

    0

    0; ;V

    " VI " I R "R

    = = =

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    E3a&ple M.E3a&ple M. A power tool is rated atA power tool is rated at N AN Awhen used with a circuit that proideswhen used with a circuit that proides

    42"[email protected]"1@.+hat power is used in operatin'+hat power is used in operatin'this tool8this tool8

    E3a&ple 5.E3a&ple 5. A M""1+ heater draws aA M""1+ heater draws acurrent of 4" A. +hat is the resistance8current of 4" A. +hat is the resistance8

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    Su&&ary of Bor&ulasSu&&ary of Bor&ulas

    QIt

    =QIt

    = 1C1 A1 s

    =1C1 A1 s

    =Electriccurrent%Electriccurrent%

    ; ;V V

    I V IR R

    R I

    = = =; ;V V

    I V IR R

    R I

    = = =

    #h&s Gaw#h&s Gaw

    1 volt-esistance: 1 oh!

    1 a!pere=

    1 volt-esistance: 1 oh!

    1 a!pere=

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    Te&perature coe-cient ofresistance%

    Te&perature coe-cient ofresistance%

    Su&&ary =Cont.>Su&&ary =Cont.>

    orL RARA L

    = = orL RARA L

    = =

    /

    /

    1; #nits:

    C

    R

    R t

    =

    /

    /

    1; #nits:

    C

    R

    R t

    =

    00; ;

    V" VI " I R "

    R= = =

    00; ;

    V" VI " I R "

    R= = =

    /R R t =

    ResistiityResistiityofof

    &aterials%&aterials%

    ResistiityResistiityofof

    &aterials%&aterials%

    ElectricPower P:

    ElectricPower P:

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    C#OCGUS#O% Chapter 27C#OCGUS#O% Chapter 27

    Current and ResistanceCurrent and Resistance


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