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University of Khartoum -Signals and Systems- Lecture 11
بسم الله الرحمن الرحيم University of Khartoum -Signals and Systems- Lecture 11 2015 University of Khartoum Department of Electrical and Electronic Engineering Third Year Signals and Systems Lecture 15: Laplace Transform Dr. Iman AbuelMaaly Abdelrahman Course Specifications
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Outline Signal Transforms Laplace Transform Region of Convergence
Pole-Zero Plot Exercises 2015
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Signals Transform DSP DSP Signal in time domain x(t)
Continuous-Time signals Discrete-Time signals Signal in time domain x(t) Signal in time domain x[n] Signal in frequency domain - Fourier Series Ck - Fourier Transform X(jω) Signal in frequency domain - Fourier Series Ck Fourier Transform X(ejω) DSP Signal in Laplace domai Laplace Transform X(s) Signal in Z- domain - Z- Transform X(Z) DSP
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The Laplace Transform Assume s is any complex number of form: s = + j That is, s is not purely imaginary and it can also have real values. X(s)|s=j=X(j). X(s) is called the Laplace transform of x(t) 2015
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Laplace Transform In general, for a signal x(t): Is the bilateral Laplace transform, and Is the unilateral Laplace transform.
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Laplace Transform ( S-Plane)
The xy-axis plane, where x-axis is the real axis and y-axis is the imaginary axis, is called the s-plane. Im (S) Re (S)
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Laplace Transform Fourier transform is the projection of Laplace transform on the imaginary axis on the s-plane. This gives two additional flexibility issues to the Laplace transform: Analyzing transient behavior of systems Analyzing unstable systems
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Region of Convergence (ROC)
Similar to the integral in Fourier transform, the integral in Laplace transform may also not converge for some values of s. So, Laplace transform of a function is always defined by two entities: Algebraic expression of X(s). Range of s values where X(s) is valid, i.e. region of convergence (ROC). 2015
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Region of Convergence (ROC)
The ROC consists of those values of for which the Fourier Transform of Converges 2015
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The Laplace Transform Transform techniques are an important tool in the analysis of signals and LTI systems. The Z-transform plays the same role in the analysis of discrete-time signals and LTI systems as the Laplace transform does in the analysis of continuous-time signals and systems.
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Example (L-Transform)
Compute the Laplace Transform of the following signal: For what values of a X(s) is valid? 2015
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Obtain the Fourier Transform of the signal
(1)
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Laplace Transform or with 2015
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By comparison with Eqn (1) we recognized Eqn(1) as the Fourier Transform of
And Thus, 2015
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Or equivalently, since and
And thus That is, 2015
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2015
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Example 2 2015
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t
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2015
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Pole-Zero Plot Given a Laplace transform
Poles of X(s): are the roots of D(s). - Zeros of X(s): are the roots of N(s). 2015
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Example3 Find X(s) for the following x(t). 2015
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The set of values of Re{s} for which the Laplace transforms of both terms converges is Re{s} >-1, and thus combining the two terms on the right hand side of the above equation we obtain: 2015
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Has poles at p1 =-1 and p2 =-2 and a zero at z =1
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Im ROC S-plane X X -2 -1 1 Re pole zeros
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Inverse Laplace Transform
Integral of inverse Laplace transform: However, we will mainly use tables and properties of Laplace transform in order to evaluate x(t) from X(s). That will frequently require partial fractioning.
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Laplace Transform and LTI
x(t)=est y(t)=h(t)* est In the above system, H(s) is called the transfer function of the system. It is also known as Laplace transform of the impulse response h(t). LTI 2015
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System Characterization by LT
x(t) Causality Stability h(t) y(t)
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