Engineering Circuit Analysis-CH8

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    Engineering Circuit AnalysisEngineering Circuit Analysis

    CH8 Fourier Circuit AnalysisCH8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series8.2 Use of Symmetry8.2 Use of Symmetry

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    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

    - Most of the functions of a circuit are periodic functions

    - They can be decomposed into infinite number of sine and

    cosine functions that are harmonically related.

    - A complete responds of a forcing function =

    Partial response to each harmonics.∑ erpositonsup

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    Harmonies: Give a cosine function

    -  : fundamental freuency ! is the fundamental "ave form#

    - Harmonics have freuencies

    ( )

    $

    $

    $%

    &%:

    &:

    cos&

    w f  T T 

    w f   f  

    t wt v

    π 

    π 

    ==

    ==

    $w   ( )t v%

    ( )   t nwat v nn $cos=

    Amplitude of the nth harmonics

    !amplitude of the fundamental "ave form#

    '(')'&' $$$$   wwww

    *re. of the %st harmonics

    !=fund. fre#

    *re. of the &nd 

    harmonics

    *re. of the nthharmonics

    *re. of the )rd harmonics

    *re. of the (th harmonics

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

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    8.1 Fourier Series8.1 Fourier Series Example *undamental: v

    %

     = &cosw$

    v)a = cos)w$t  v)b = %.+cos)w$t 

    v)c = sin)w$t 

    Ch8 Fourier Circuit Analysis

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    - *ourier series of a periodic function

      Given a periodic function

    can be represented by the infinite series as

    ! # ! # ! #T t  f  t  f  t  f     ,=:

    ( )t  f  

    ( )

    ( )∑∞

    =

    ++=

    ++++++=

    %

    $$$

    $&$%

    $&$%$

    sincos

    &sinsin&coscos

    n

    nn   t nwbt nwaa

    t wbt wbt wat waat  f  

    $

    =

    =

    =

    n

    n

    b

    a

    a

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

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    /ample %&.%

    ( )

    ≤≤

    ≤≤−==

    ).$%.$'$

    %.$%.$'+cos

    t t V t V 

      m   π 

    π 

    mV 

    a  =$

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

    Given a periodic function

    0t is 1no"ing

    &%

    mV 

    a =

      ( )( )%n % &

    cos&&   >−= n

    nV 

    a   mn

    π 

    π  $$=b

    0t can be seen ' "e can evaluateπ ω  +$=

    π )

    &&

    mV a   =   $)=a

    π %+

    &(

    mV a   −=   $+=a

    π )+

    &2

    mV a   =

    ( )

    ++

    −++=

    t V 

    t V 

    t V 

    t V V 

    t V 

    m

    mmmm

    π 

    π 

    π π 

    π π 

    π π 

    )$cos

    )+

    &$cos%+

    &%$cos

    )

    &+cos

    &

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    -3evie" of some trigonometry integral observations

    !a#

    !c#

    !d#

    $sin$

    $   =∫    dt t nwT 

    $cos$

    $   =∫    dt t nwT 

    !b#

    !e#

    ( ) ( )[ ] $sinsin&

    %cossin

    $$$

    $$$   =−++= ∫ ∫    dt t wnk t wnk dt t nwt kw

    T T 

    ( ) ( )[ ]

    ==

    +−−=

    ∫ 

    ∫ 

    nk if  

    nk if  T 

    dt t wnk t wnk 

    dt t nwt kw

    '$

    '&

    coscos&

    %

    sinsin

    $   $$

    $  $$

    ( ) ( )[ ]

    ==

    ++−=

    ∫ 

    ∫ 

    nk if  

    nk if  T 

    dt t wnk t wnk 

    dt t nwt kw

    '$

    '&

    coscos&

    %

    cossin

    $   $$

    $  $$

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

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    -valuations of    nn   baa   ''$

    $a   ( ) ( )∫  ∑∫ ∫   ∞

    =

    ++=  T 

    n

    nn

    T T 

    dt t nwbt nwadt adt t  f  $

    %

    $$$

      $$

    sincos

    4ased on !a# !b#

    ( ) $sincos$

    %

    $$   =+∫  ∑∞

    =

    n

    nn   dt t nwbt nwa   ( )∫ =  T 

    dt t  f  T 

    a$

    $

    %

    $a! is also called the 56 component of #( )t  f  

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

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    na

    4ased on !b#

    ( )

    ∫  ∑

    ∫  ∑∫ ∫ ∞

    =

    =

    +

    +=

    n

    n

    n

    nT T 

    dt t kwt nwb

    dt t kwt nwadt t kwatdt kwt  f  

    $%

    $$

    $%

    $$$

      $$$

      $

    cossin

    coscoscoscos

    ( )∫ 

    ∫  ∑

    =

    =∞

    =

    n

    n

    n

    n

    tdt nwt  f  T 

    a

    aT 

    dt t kwt nwa

    $  $

    $%

    $$

    cos&

    &coscos

    $cossin$

    %

    $$   =∫  ∑∞

    =

    n

    n   dt t kwt nwb

    $cos$

    $$   =∫    dt t kwaT 

    4ased on !c#

    4ased on !e#

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

    7hen k =n

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    nb

    4ased on !a#

    ( )

    ∫  ∑

    ∫  ∑∫ ∫ ∞

    =

    =

    +

    +=

    n

    n

    n

    n

    T T 

    dt t kwt nwb

    dt t kwt nwadt t kwatdt kwt  f  

    $%

    $$

    $%

    $$$

      $$$

      $

    sinsin

    sincossinsin

    ( )∫ 

    ∫  ∑

    =

    =∞

    =

    n

    n

    n

    n

    tdt nwt  f  T 

    b

    bT 

    dt t kwt nwb

    $  $

    $%

    $$

    sin&

    &sinsin

    $sincos$

    %

    $$   =∫  ∑∞

    =

    n

    n   dt t kwt nwa

    $sin$

    $$   =∫    dt t kwaT 

    4ased on !c#

    4ased on !d#

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

    7hen k =n

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    ( )nnnnn   t nwbat nwbt nwa   φ ++=+ $&&

    $$   cossincos

    #! Hz  f  

    &&

    nnn   bav   +=

    Harmonicamplitude

    8v

    $8 f  $2 f  $+ f  $( f  $) f  $& f  $ f  

    +v

    2v

    (v)v&v%v

    Phase spectrum

    $

     f  $

    & f  $

    ) f  $

    ( f  $

    + f  $

    2 f  $

    8 f    #! Hz  f  

    n

    φ 

    n

    nn

    ab−=   −%tanφ 

    Ch8 Fourier Circuit Analysis

    8.1 Fourier Series8.1 Fourier Series

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    - 5epending on the symmetry !odd or even#' the *ourier series can be further simplified.

     Even Symmetry

    Observation: rotate the function curve along a/is' the curve

    "ill overlap "ith the curve on the other half of .

    /ample :

    Odd Symmetry

    Observation: rotate the function curve along the a/is' then along

    the a/is' the curve "ill overlap "ith the curve on the other

    half .

    /ample :

    ( ) ( )t  f  t  f     −=

    ( ) ( )t  f  t  f     −−=

    ( )   wt t  f   cos=

    ( )t  f  

    ( )t  f  

    ( )   wt t  f   sin=

    ( )t  f  

    Ch8 Fourier Circuit Analysis

    8.2 Use of Symmetry8.2 Use of Symmetry

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    9ymmetry Algebra

    !a# odd func. =odd func. × even func.

    /ample:

     

    !b# even func. =odd func. odd func.

    /ample:

    !c# even func. =even func. even func./ample:

    t ωt ωt ω

    cossin=&

    &sin

    t ωt ωt ω

    coscos=&

    %,&cos

    t ωt ωt ω

    sinsin=&

    &cos-%

    Ch8 Fourier Circuit Analysis

    8.2 Use of Symmetry8.2 Use of Symmetry

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    !d# even func. =const. ,∑ even func. !;o odd func.#

    /ample:

     

    !e# odd func. =∑odd func.

    /ample:

    t ωt ωt ω && sin&-%=%-cos&=&cos

    ! #   φt ωφt ωφt ω sincos,cossin=,sin

    odd func. odd func.

    Ch8 Fourier Circuit Analysis

    8.2 Use of Symmetry8.2 Use of Symmetry

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    Apply the symmetry algebra to analy

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    Half-"ave symmetry  f  !t # = - f  !t  - # or  f  !t # = - f  !t  , #&T  &

    Ch8 Fourier Circuit Analysis

    8.2 Use of Symmetry8.2 Use of Symmetry

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    ( )

    ( )

    =

    =

    ∫ 

    ∫ 

    evenisn

    odd isntdt nwt  f  T b

    evenisn

    odd isntdt nwt  f  

    T a

    n

    n

    $

    sin(

    $

    cos(

    $

    $

    $

    $

    *ourier series:

    Ch8 Fourier Circuit Analysis

    8.2 Use of Symmetry8.2 Use of Symmetry