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    1

    Basic Laws

    Discussion D2.1

    Chapter 2Sections 2-1 2-6, 2-10

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    2

    Basic Laws

    Ohm's Law

    Kirchhoff's Laws

    Series esistors an! "o#ta$e Di%ision

    &ara##e# esistors an! Current Di%ision

    Source (chan$e

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    )

    Georg Simon Ohm*1+ 1/

    httpwww-histor3.4cs.st-an!rews.ac.u5histor3&ictDisp#a3h4.ht4#

    7er4an professor who pu8#ishes a 8oo5

    in 12+ that inc#u!es what is now 5nown

    as h4's #aw.

    h4's Law 9he %o#ta$e across a resistor

    is !irect#3 proportiona# to the currect

    f#owin$ throu$h it.

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    /

    esistance

    A

    l: #en$th

    esistance R l A=

    = resisti%it3 in h4-4eters

    7oo! con!uctors *#ow Copper, 7o#!

    7oo! insu#ators *hi$h 7#ass, &aper

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    h4's Law

    v iR= viR

    =

    ;nits of resistance, R, is h4s *

    vRi

    =

    R: 0 short circuit R= open circuit

    1v i R= 1* i i=

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    6

    ;nit of 7 is sie4ens *S,

    Con!uctance, 7

    1G

    R=

    iv

    G= i Gv=

    iG

    v=

    1 S : 1

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    +

    &ower

    < resistor a#wa3s !issipates ener$3= it transfor4s

    e#ectrica# ener$3, an! !issipates it in the for4 of heat.

    ate of ener$3 !issipation is the instantaneous power2

    2 * * * * * 0v t

    p t v t i t Ri tR

    = = =

    22 * * * * * 0

    i tp t v t i t Gv t

    G= = =

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    Basic Laws

    h4's Law

    Kirchhoff's Laws

    Series esistors an! "o#ta$e Di%ision

    &ara##e# esistors an! Current Di%ision

    Source (chan$e

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    7usta% o8ert Kirchhoff *12/ 1+

    httpwww-histor3.4cs.st-an!rews.ac.u5histor3&ictDisp#a3Kirchhoff.ht4#

    Born in &russia *now ussia, Kirchhoff

    !e%e#ope! his >#aws> whi#e a stu!ent in

    1/. 9hese #aws a##owe! hi4 to

    ca#cu#ate the %o#ta$es an! currents in4u#tip#e #oop circuits.

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    10

    CIRCUIT TOPOLOGY

    Topology ?ow a circuit is #ai! out.

    < branchrepresents a sin$#e circuit *networ5

    e#e4ent= that is, an3 two ter4ina# e#e4ent.

    < noeis the point of connection 8etween two or4ore 8ranches.

    < loopis an3 c#ose! path in a circuit *networ5.

    < #oop is sai! to 8e inepenen! if it contains a8ranch which is not in an3 other #oop.

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    11

    @un!a4enta# 9heore4 of Aetwor5 9opo#o$3

    1b l n= +

    @or a networ5 with b8ranches, nno!es

    an! lin!epen!ent #oops

    (a4p#e

    b

    =n=

    l=

    "

    #

    #

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    1/

    Kirchoff$s C%rren! Law*KCL

    9he a#$e8raic su4 of the currents enterin$ a

    no!e *or a c#ose! 8oun!ar3 is ero.

    1

    0N

    n

    n

    i=

    =

    where N: the nu48er of 8ranches connecte! to

    the no!e an! in : the nth current enterin$

    *#ea%in$ the no!e.

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    1

    1

    0N

    n

    n

    i

    =

    =1i

    .i

    2i

    )i

    /i

    Sign con&en!ion Currents enterin$ the no!e are positi%e,

    currents #ea%in$ the no!e are ne$ati%e.

    1 2 ) / 0i i i i i+ + =

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    16

    Kirchoff$s C%rren! Law*KCL

    9he a#$e8raic su4 of the currents enterin$

    *or #ea%in$ a no!e is ero.

    1i

    .i

    2i

    )i

    /i1 2 ) / 0i i i i i+ + =

    1 2 ) / 0i i i i i + + =

    9he su4 of the currents enterin$ a no!e iseua# to the su4 of the currents #ea%in$ a no!e.

    1 2 / ) i i i i i+ + = +

    nterin$

    Lea%in$

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    1+

    Kirchoff$s ol!age Law*K"L

    9he a#$e8raic su4 of the %o#ta$es aroun!

    an3 #oop is ero.

    1

    0M

    m

    m

    v=

    =

    where M : the nu48er of %o#ta$es in the #oop

    an! vm: the mth%o#ta$e in the #oop.

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    1

    Sign con&en!ion 9he si$n of each %o#ta$e is the po#arit3 of the

    ter4ina# first encountere! in tra%e#in$ aroun! the #oop.

    9he !irection of tra%e# is ar8itrar3.

    C#oc5wise

    Counter-c#oc5wise

    0 1 2 0V V V + + =

    2 1 0 0V V V + =

    0 1 2V V V= +

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    1

    Basic Laws

    h4's Law

    Kirchhoff's Laws

    Series Resis!ors an ol!age (i&ision

    &ara##e# esistors an! Current Di%ision

    Source (chan$e

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    20

    0 1 2 1 2V V V IR IR= + = +

    ( )1 2I R R= +

    sIR=

    1 2sR R R= +

    Series Resis!ors

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    21

    V0

    I

    R1

    R2

    V1

    V2

    A

    ol!age (i&ier

    0 0

    1 2s

    V VI

    R R R= =

    +

    ( )02 2 2

    1 2

    VV IR RR R= = +

    ( )2

    2 0

    1 2

    R

    V VR R= +

    ( )1

    1 0

    1 2

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    22

    Basic Laws

    h4's Law

    Kirchhoff's Laws

    Series esistors an! "o#ta$e Di%ision

    Parallel Resis!ors an C%rren! (i&ision

    Source (chan$e

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    2)

    VR

    1

    I

    R2

    I1 I2

    1 2

    1 2

    V VI I I

    R R= + = +

    Parallel Resis!ors

    1 2

    1 1V

    R R

    = +

    p

    V

    R=

    1 2

    1 1 1

    pR R R= +

    1 2

    1 2

    p

    R RR

    R R=

    +

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    2/

    Current Di%ision

    1 2

    1 2

    * * * p

    R Rv t R i t i t

    R R= =

    +

    21

    1 1 2

    * * * Rv ti t i t R R R

    = =+

    1

    2

    2 1 2

    *

    * *

    Rv t

    i t i t R R R= = +

    C%rren! i&ies in in&erse propor!ion !o !he resis!ances

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    2

    Current Di%ision

    Nresistors in para##e#

    1 2

    1 1 1 1

    p nR R R R

    = + + + * * p

    v t R i t =

    * * *

    p

    j

    j j

    Rv ti t i t

    R R= =Current in jth8ranch is

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    26

    Basic Laws

    h4's Law

    Kirchhoff's Laws

    Series esistors an! "o#ta$e Di%ision

    &ara##e# esistors an! Current Di%ision

    So%rce )*change

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    2+

    Source (chan$e

    +e can always replace a &ol!age so%rce in series wi!h a

    resis!or by a c%rren! so%rce in parallel wi!h !he same resis!or

    an &ice,&ersa-

    (oing !his. howe&er. ma/es i! impossible !o irec!ly fin !he

    original so%rce c%rren!-

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    2

    Source (chan$e &roof

    ol!age across an c%rren! !hro%gh any loa are !he same

    ( )L

    L s

    s L

    Rv v

    R R=

    +

    ( )s

    a

    s L

    vi

    R R=

    +

    ( )' s sa a

    s L s

    R vi i

    R R R= =

    +

    ( )' LL a L s

    s L

    Rv i R v

    R R= =

    +