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Using Partial Fraction Expansion
Professor Walter W. Olson Department of Mechanical, Industrial and Manufacturing Engineering University of Toledo Using Partial Fraction Expansion
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Outline of Today’s Lecture
Review Laplace Transform Inverse Laplace Transform Properties of the Laplace Transform Final Value Theorem
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Laplace Transform Traditionally, Feedback Control Theory was initiated by using the Laplace Transform of the differential equations to develop the Transfer Function The was one caveat: the initial conditions were assumed to be zero. For most systems a simple coordinate change could effect this If not, then a more complicated form using the derivative property of Laplace transforms had to be used which could lead to intractable forms While we derived the transfer function, G(s), using the convolution equation and the state space relationships, the transfer function so derived is a Laplace Transform under zero initial conditions
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Laplace Transform CAUTION: Some Mathematics is necessary!
The Laplace transform is defined as Fortunately, we rarely have to use these integrals as there are other methods
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Some Common Laplace Transforms
The Laplace Transform of the Impulse Function The Laplace Transform of the Step Function The Laplace Transform of a Unit Ramp: The Laplace Transform of the 2nd power of t: The Place Transform of the nth power of t:
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Some Common Laplace Transforms
Laplace Trans Form of the exponentials: Laplace Transforms of trigonometric functions:
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Important Inverse Transforms
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Properties of the Laplace Transform
Laplace Transforms have several very import properties which are useful in Controls Now, you should see the advantage of having zero initial conditions
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Final Value Theorem If f(t) and its derivative satisfy the conditions for Laplace Transforms, then This theorem is very useful in determining the steady state gain of a stable system transfer function Do not apply this to an unstable system as the wrong conclusions will be reached!
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The Transfer Function
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Partial Fraction Expansion
When using Partial Fraction Expansion, our objective is to turn the Transfer Function into a sum of fractions where the denominators are the factors of the denominator of the Transfer Function: Then we use the linear property of Laplace Transforms and the relatively easy form to make the Inverse Transform.
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Partial Fraction Expansion
There are three cases that we need to consider in expanding the transfer function: Case 1: All of the roots are real and distinct Case 2: Complex Conjugate Roots Case 3: Repeated roots
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Case 1: Real and Distinct Roots
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Case 1: Real and Distinct Roots Example
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Case 1: Real and Distinct Roots An Alternative Method (usually difficult)
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Case 1: Real and Distinct Roots Example
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Case 2: Complex Conjugate Roots
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Case 2: Complex Conjugate Roots Example
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Case 3: Repeated Roots
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Case 3: Repeated Roots Example
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Heaviside Expansion
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State Space Formulation
Example: The Nose Wheel
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Example Now, we have a good view of the system structure
so that we can choose and adjust values, if needed
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Example
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Summary Next Class: Nyquist Stability Criteria
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