s Plane Review

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  • 7/27/2019 s Plane Review

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    EE122, Stanford University, Ross Venook

    S-plane Explained

    Introduction

    Motivation for s-plane analysis

    When I say s-plane, what do I mean?

    How to use the s-plane

    Circuit analysis/design: the Integrator

    Signal analysis/design: FM

    A (P)REVIEW OF LAPLACE TRANFORMS AND

    HOW TO USE THEM IN EE122

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    EE122, Stanford University, Ross Venook

    Motivation for s-plane analysis

    Understanding circuits in another

    domain (the frequency domain) The more ways we can understand our

    circuit, the better because...

    The time domain is hard for some things

    filtering = convolution (Doh!)

    The s-plane (often) makes things easier

    filtering = multiplication (Woohoo!)

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    EE122, Stanford University, Ross Venook

    Math behind the s-plane

    The actual Laplace Transform*:

    h(t) could be a signal, or a system As a signal:

    As a system:

    H(s): Laplace Transform of h(t)

    s = + j: Complex Frequency Variable

    *: not necessary for EE122, but interesting (maybe)

    =

    0)()( dtethsH st

    )16.015sin()( += tth

    )(

    )()(

    tv

    tvth

    in

    out=

    The Laplace Transform of a time-domain function gives us

    a function of the complex frequency variable s

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    EE122, Stanford University, Ross Venook

    A note about transforms

    They make life easier (or should)

    If youve taken E40 (and/or Math 53),

    you have already used transforms

    E40 uses phasor analysis of linear circuits

    Complex impedances are just a tricky way ofgetting around differential equations so that we

    can take C as a resistor of value 1/ jC.

    Indeed, they are simply Laplace (or Fourier)transforms in disguise--as you will see.

    Math 53 uses Laplace Transforms to solve

    differential equations

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    EE122, Stanford University, Ross Venook

    What do I mean when I say s-plane?

    Example:

    Tent pole plot of the

    magnitude of a

    Chebychev filters

    response to inputs ofcomplex frequency s

    is what you usually

    think of as radianfrequency (=2f)

    is decay rate*

    ANSWER: THE REAL () AND IMAGINARY () PARTS OF s

    ARE THE x and y ON A GRAPH

    *: Not important for EE122, but used in stability analysis

    -axis axis s-plane

    |H(s)|

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    EE122, Stanford University, Ross Venook

    Why should I use the s-plane?

    Turns differential equations (hard) into

    algebraic equations (easy)

    Turns convolution (hard) into multiplication

    (easy)

    THIS IS THE SAME QUESTION AS:WHY IS THE LAPLACE TRANSFORM USEFUL?

    inoutinoutout CvvsBAtCvdtdvBtAv =+=+ )()()(

    sBACsH

    vv

    in

    out

    +== )(

    )()()()()()( sGsHsFtgthtf ==

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    EE122, Stanford University, Ross Venook

    How to use s-plane analysis

    Examples to follow:

    Systems Simple RC circuit

    Integrator

    Signals

    Multiplication by a sinusoid: Heterodyning

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    EE122, Stanford University, Ross Venook

    RC circuit (simple)

    Straight from EE122 lecture notes:

    sRCsH

    vv

    vsRCv

    TransformLaplaceMagictvdtdvRCtv

    dtdvCi

    iRtvtverivation

    in

    out

    inout

    inoutout

    out

    inout

    +==

    =+

    =+

    =

    =

    11)(

    )1(

    )("")()(

    )()(:

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    EE122, Stanford University, Ross Venook

    Integrator (slightly less simple)

    121

    2

    2211

    21

    1

    2

    )(

    )(

    )//)(()(

    /)(

    /)()(

    ))()(()(

    :

    RCRsR

    RsH

    v

    v

    RvvCRsRR

    RdtCdvRtvtv

    dtCdvti

    Rtvti

    Rtititv

    AnalysisC

    in

    out

    inout

    outinout

    outC

    inin

    Cinout

    +==

    =+

    +=

    =

    =

    =

    1

    2

    2

    1

    R

    R

    CR2

    1

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    EE122, Stanford University, Ross Venook

    A familiar slide

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    Another familiar slide...

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    A last familiar slide

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    EE122, Stanford University, Ross Venook

    Heterodyning (for FM radio)

    Motivation: Base-band txn is trouble Efficiency

    /4 Antenna for kHz ~ length > kilometers Interference

    All of the signals would muddle together

    Hence, we need distinct carrierfrequencies (regulated by the FCC)

    92.3 MHz (KSJO)

    88.5 MHz (KQED)

    1070 kHz (KNX)

    710 kHz (KABC)

    FM

    AM

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    EE122, Stanford University, Ross Venook

    The frequency domain

    All base-band:

    Heterodyned

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    EE122, Stanford University, Ross Venook

    Back to heterodyning

    Because convolution in the time domain is multiplicationin the frequency domain, when we multiply by a sinusoid

    in the time domain, it convolves the frequency content of

    our signal up to the frequency of the sinusoid.(Whew! That was a mouthful)

    Base-band signal...

    convolved with pure tone...

    yields heterodyned signal!

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