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    Filter Design/1

    Frequency Response of Filters

    An important group of systems are filters. The

    characteristics of a filter are shown by its response to

    sinusoids of various frequencies.

    Example, the spectral content of speech over telephone

    channel 300 3100 Hz. A filter that limits the spectrum

    of the signal is used.

    A filter has a passband and a stop-band frequencies and

    is classified into lowpass, highpass or bandpass types.

    The transmission of a signal must be distortionless,

    except only for a possible scaling of amplitude and aconstant time delay.

    Suppose we have a filter with response H(s). Then the

    output due to an exponential ste isstesH )( .

    Setting js = , we gettjtj ejHe )( and tjtj ejHe )( .

    From these,

    ])(Re[2

    )()()cos(2

    tj

    tjtj

    ejH

    ejHejHt

    +

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    We can express )( jH in polar form as

    )(|)(|)( jHejHjH = .

    The response due to the input ttf cos)( = is then

    )](cos[|)(|)( jHtjHty += .

    Similarly, the output due to the input )cos()( += ttf

    can be shown to be given by

    )](cos[|)(|)( jHtjHty ++=

    Note that the result is valid only for stable systems as we

    have set js = . For marginally stable and unstable

    systems, the convergence region does not include the

    imaginary axis.

    We see that a sinusoid of frequency when passed

    through a filter will have its amplitude increase by

    |)(| jH and its phase shifted by )( jH .

    |)(| jH is called the amplitude response of the filter, and

    )( jH is called the phase response. Both of them

    together form the frequency response of the filter.

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    Example: (a) Find the frequency response of a system

    with5

    1.0)(

    ++

    =s

    ssH .

    (b) Find the output if input is )5010cos( t .

    a) Amplitude response25

    01.0|)(|

    2

    2

    +

    +=

    jH

    Phase response =

    5tan

    1.0tan)( 11

    jH

    b) For input )5010cos( +t , 894.025100

    01.0100|)10(| =

    ++

    =jH

    =

    = 26

    5

    10tan

    1.0

    10tan)( 11jH

    so )265010cos(894.0)( += tty

    = 0.894cos(10t- 24).

    Causal Sinusoidal Inputs

    Now we consider the case of the causal sinusoid. First

    we look at the causal exponential input )()( tuetf tj= .

    Then -

    jssF

    =

    1)( .

    The output is given by

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    ))()...()((

    )()(

    )(

    )()()()(

    21 jssss

    sPsF

    sQ

    sPsHsFsY

    n ===

    where n are the natural roots of the system

    characteristic eqn.

    Suppose the partial fraction expansion of the right hand

    term yields coefficients nkkk ,...,, 21 for

    )),..((),( 21 nsss . The coefficient corresponding to

    the last term )( js is -

    )()(

    )(

    jHsQ

    sP

    js

    ==

    .

    Hence

    = +

    =

    n

    i i

    i

    js

    jH

    s

    ksY

    1

    )()(

    and =

    +=n

    i

    tjti ejHtuekty

    i

    1

    )()()(

    .

    For a stable system, all the characteristic modes will

    decay to 0, and thus the steady state output from a

    causal sinusoid is also )](cos[|)(|)( jHtjHty += .

    Bode Plots

    The amplitude and phase response plot of a system can

    be sketched easily if we use a logarithmic scale for.

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    Such plots are called Bode plots, and the approach uses

    the asymptotic behavior of the amplitude and the phase

    responses.

    Consider the transfer function

    ))((

    ))(()(

    322

    1

    21

    bsbsbss

    asasKsH

    +++++

    =

    where 322 bsbs ++ has complex conjugate roots.

    Rewriting it,

    ++

    +

    +

    +

    =11

    11

    )(

    3

    2

    3

    2

    1

    21

    31

    21

    sb

    b

    b

    s

    b

    ss

    a

    s

    a

    s

    bb

    aKasH .

    Thus, in terms of frequency,

    ++

    +

    +

    +

    =

    3

    2

    3

    2

    1

    21

    31

    21

    )(11

    11

    )(

    b

    j

    b

    bj

    b

    jj

    a

    j

    a

    j

    bb

    aKajH

    .

    The amplitude response is the quotient of the product of

    the absolute values of the complex terms. The phase

    response is just the sum of phases of each term in

    numerator minus the sum of the phases of each term in

    the denominator.

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