Lecture 6 Modelling Second Order Systems and Examples
Process Control
- Prof. Kannan M. Moudgalya
IIT Bombay Wednesday, 31 July 2013
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Lecture 6 Modelling Second Order Systems and Examples Process - - PowerPoint PPT Presentation
Lecture 6 Modelling Second Order Systems and Examples Process Control Prof. Kannan M. Moudgalya IIT Bombay Wednesday, 31 July 2013 1/39 Process Control Second Order Models and Response Outline 1. Poles, zeros, response for different pole
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◮ Let the transfer function be G(s) = N(s)/D(s)
◮ The roots of N(s) = 0 are called zeros of G(s) ◮ The roots of D(s) = 0 are called poles of G(s)
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◮ Let the transfer function be G(s) = N(s)/D(s)
◮ The poles of 1 + KG(s) are
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◮ Let the transfer function be G(s) = N(s)/D(s)
◮ Let the closed loop transfer function be T(s):
◮ The poles of T(s) are
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◮ Y(s) =
n
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◮ Y(s) =
n
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◮ For the pole at a
◮ The exponential part
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1
2 G a = 1/( s +3) 3
4
5
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◮ For the pole at a
◮ The exponential part
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1
2 G b = 1/( s −2) 3
4
5
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◮ For the poles at
◮ There will be growing
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1
2 G c = 1/( s −(1+2∗%i) ) /( s −(1−2∗%i) ) 3
4
5
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◮ For the poles at
◮ There will be
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1
2 G d = 1/( s −(−1+3∗%i) ) /( s −(−1−3∗%i) ) 3
4
5
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◮ Y(s) = G(s)U(s), G(s) =
◮ τ is the time constant ◮ ζ is the damping coefficient ◮ K is the steady state gain ◮ Step response: Y(s) =
◮ =
◮ Is there a relation between a and b, A and B? ◮ For ζ < 1, a = b∗, A = B∗
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◮ Y(s) =
◮ a and b are roots of τ 2s2 + 2ζτs + 1 = 0 ◮ a, b = −2ζτ ±
◮ = −ζ
◮ ζ ≥ 1, a, b are real ◮ ζ < 1, complex, a = b∗, A = B∗
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◮ Known as an overdamped system (ζ > 1) ◮ Its solution is given by
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◮ Known as critically damped system (ζ = 1) ◮ Its solution is given by
Process Control Second Order Models and Response
◮ Known as underdamped system (ζ < 1) ◮ Its solution is given by
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n
n
◮ K is taken as 1 ◮ ωn: natural frequency, ζ: damping factor. ◮ For different ζ, get underdamped (ζ < 1),
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n
n
Process Control Second Order Models and Response
Mp
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1
2
3 omegan = 1 ;
4 y = second ( omegan , 0 . 1 , t ) ; 5 y = second ( omegan , 0 . 5 , t ) ; 6 y = second ( omegan , 1 , t ) ; 7 y = second ( omegan , 2 , t ) ; 1
2 G = omegan ˆ2/( s ˆ2+2∗ zeta ∗omegan∗ s+
3 y = csim ( ’ step ’ , t ,G) ; 4
5
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◮ Adh
◮ In deviational variables, ◮ Ad∆h
◮ Taking Laplace transform,
◮ ∆h(s) =
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◮ Y(s) =
◮ Multiply by τs + 1, let s = −1/τ, A = Kaτ 2 ◮ Multiply by s2: ◮
◮ By letting s = 0, C = Ka ◮ Differentiating blue equation w.r.t. s ◮ and letting s = 0, B = −Kaτ
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◮ Y(s) =
◮ Y(s) = Kaτ 2
◮ Inverting ◮ y(t) = Kaτ
◮ y(t = ∞) = Ka(t − τ) ◮ Let K = 1 and plot u(t) and y(t) in the same
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◮ Give the following input, u(t):
◮ u(t) = 1(t) × M − 1(t − t1) × M ◮ 1(t) denotes unit step input ◮ u(t) = [1(t) − 1(t − t1)] × M ◮ U(s) =
◮ U(s) = [1 − e−t1s] M
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◮ Poles, zeros, response of systems for different
◮ Solution to second order systems ◮ Integrating or capacitive systems
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