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Published byKerrie Stafford Modified over 9 years ago
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Modeling Transient Response So far our analysis has been purely kinematic: The transient response has been ignored The inertia, damping, and elasticity of the plant have been ignored But – no more!
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Writing the Equations of Motion The prototypical second order system is the mass spring damper. Let’s analyze this system: Force exerted by the spring: Force exerted by the damper: Force exerted by the inertia of the mass:
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Consider the motion of the mass there are no other forces acting on the mass therefore, the equation of motion is the sum of the forces: Why is this a linear system? Writing the Equations of Motion
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Your finger Suppose that your finger “plucks” the mass (i.e. applies a dirac delta transient force): Writing the Equations of Motion
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Write the equation of motion for a torsional damped inertia: For example, a rotating shaft with friction Writing the Equations of Motion: Example 1 Torque due to inertia: Torque due to damping:
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Write the equations of motion for the following: assume a frictionless joint Writing the Equations of Motion: Example 2
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Write the equations of motion for the following: Writing the Equations of Motion: Example 3
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The Laplace Transform How does the mass respond to the transient force? You have to solve this differential equation: We will analyze it using the Laplace transform: And the inverse Laplace transform:
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The Laplace Transform: Properties Linearity: Frequency shift: Time shift: Scaling:
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The Laplace Transform: Properties Differentiation: Integration: Final value theorem:
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The Laplace Transform: Examples Step function: Ramp function:
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Given:, find The Laplace Transform: Examples
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Given:, find SMD Laplace Transform
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SMD Transform The Laplace transform of the SMD equation of motion: SMD transfer function: Multiplying by this expression converts forces to displacements in the frequency domain This is called the “characteristic equation” of the transfer function.
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SMD Transform
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System Transform: Example Write the transform for the following system:
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System Transform: Example Write the transform from to for the following system: Assume: The block experiences friction has no mass or friction
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Time out for partial fraction expansion! for some values of Suppose you have the following: You can always decompose the denominator as follows: You have to solve for these constants (you don’t need to know how for this course).
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SMD Transient Response: Example Note that the transient response decomposes into two exponentials The one dominates…
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SMD Transient Response: Example If you reduce damping term, then the mass will oscillate: Note that in this case, the characteristic equation has complex roots:
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SMD Transient Response: Example Remember Euler’s identity: The roots have an imaginary component:
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SMD Transient Response: Example (corrected) Frequency domain: Time domain:
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SMD Transient Response: Example (corrected) The bottom line: imaginary roots in the characteristic equation indicate that the system will oscillate.
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How do we characterize the transient response? The poles of are the roots of the denominator The zeros of are the roots of the numerator Pole-Zero Plot The complex plane Imaginary axis Real axis Consider the following transfer fn:
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Transient Response Different negative real poles correspond to non-oscillatory exponential decay Overdamped Im Re Overdamped Critically damped
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Transient Response Repeated negative real poles correspond to the “fastest” non-oscillatory exponential decay possible in a second order system Critically damped Im Re Im Overdamped Critically damped
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Transient Response Positive real poles correspond to non- oscillatory exponential increase Not BIBO stable Im Re
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Transient Response If there is an imaginary component to the root, then the system oscillates Underdamped Im Re
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Transient Response If the real component of a complex root is positive, then the system is not BIBO stable Im Re
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Transient Response Purely imaginary roots cause the system to oscillate forever undamped Im Re
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Second Order Transient Response Second order systems can be characterized in terms of the following: Natural frequency: the frequency of oscillation w/o damping Damping ratio: exponential decay frequency / natural frequency
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Second Order Transient Response The natural frequency is the frequency of “pure” oscillation: With a zero damping term, this becomes: Consider the transfer fn:
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Second Order Transient Response The damping ratio is: Therefore, the transfer fn can be re-written as: Damping ratio: exponential decay frequency / natural frequency
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Second Order Transient Response The damping ratio characterizes whether the second order system is underdamped, overdamped, or critically damped: underdamped critically damped overdamped If, then
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Second Order Transient Response: Example (corrected) Is the following SMD system over/under/critically damped? Therefore, it’s critically damped. If instead: then and the roots are:
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