signal and system lecture 18

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    Signals and SystemsFall 2003

    Lecture #18

    6 November 2003

    Inverse Laplace Transforms

    Laplace Transform Properties The System Function of an LTI System

    Geometric Evaluation of Laplace Transforms

    and Frequency Responses

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    Inverse Laplace Transform

    But s = +j( fixed) ds = jd

    Fix ROC and apply the inverse Fourier transform

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    Inverse Laplace Transforms Via Partial Fraction

    Expansion and Properties

    Example:

    Three possible ROCs corresponding to three differentsignals

    Recall

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    ROC I: Left-sided signal.

    ROC III: Right-sided signal.

    ROC II: Two-sided signal, has Fourier Transform.

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    Properties of Laplace Transforms

    For example:

    Linearity

    ROC at least the intersection of ROCs ofX1(s) and X2(s)

    ROC can be bigger (due to pole-zero cancellation)

    Many parallel properties of the CTFT, but for Laplace transforms

    we need to determine implications for the ROC

    ROC entire s-plane

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    Time Shift

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    Time-Domain Differentiation

    ROC could be bigger than the ROC ofX(s), if there is pole-zero

    cancellation. E.g.,

    s

    -Domain Differentiation

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    Convolution Property

    For

    Then

    ROC of Y(s) = H(s)X(s): at least the overlap of the ROCs ofH(s) &X(s)

    ROC could be empty if there is no overlap between the two ROCs

    E.g.

    ROC could be larger than the overlap of the two. E.g.

    )t(ue)t(h),t(ue)t(x tt == and

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    The System Function of an LTI System

    The system function characterizes the system

    System properties correspond to properties ofH(s) and its ROC

    A first example:

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    Geometric Evaluation of Rational Laplace Transforms

    Example #1: A first-order zero

    Graphic evaluation

    of

    Can reason about - vector length- angle w/ real axis

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    First-Order System

    Graphical evaluation ofH(j):

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    Bode Plot of the First-Order System

    -20 dB/decade

    changes by -/2

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    Second-Order System

    0 < 1

    Critically damped

    2 poles on negative real axis

    Overdamped

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    Demo Pole-zero diagrams, frequency response, and step

    response of first-order and second-order CT causal systems

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    Bode Plot of a Second-Order System

    -40 dB/decade

    Top is flat when

    = 1/2 = 0.707

    a LPF for < n

    changes by -

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    Unit-Impulse and Unit-Step Response of a Second-

    Order System

    No oscillations when

    1

    Critically (=) andover (>) damped.

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    First-Order All-Pass System

    1. Two vectors have

    the same lengths

    2.

    a

    a