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Root Locus

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Title: Elements of Feedback Control Subject: Weapons Author: Brien W. Dickson Description: 1 Hour Last modified by: Degang J. Chen Created Date: 6/4/1997 12:49:12 PM – PowerPoint PPT presentation

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Title: Root Locus


1
Root Locus
k s(sa)
y
e
r
Example

-
Two parameters k and a. would like to know how
they affect poles
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The root locus technique
  • Obtain closed-loop TF and char eq d(s) 0
  • Re-arrange terms in d(s) by collecting those
    proportional to parameter of interest, and those
    not then divide eq by terms not proportional to
    para. to get
  • this is called the root locus equation
  • Roots of n1(s) are called open-loop zeros, mark
    them with o in s-plane
  • Roots of d1(s) are called open-loop poles, mark
    them with x in s-plane

8
  • The o and x marks divide the real axis into
    several segments.
  • If a segment has an odd total number of marks to
    its right, it is part of the root locus. High
    light it.
  • If a segment has an even total number of marks,
    then its not part of root locus.
  • For the high lighted segments, mark out going
    arrows near a pole (x), and incoming arrows
    near a zero (o).

9
  • Asymptotesasymptotes order - finite zeros
    poles - finite zeros
  • n - m
  • Meeting place on the real axis at

10
  • Imaginary axis crossing point
  • From d(s) 0
  • Form Routh Table
  • Set one row 0
  • Solve for K
  • Use the row above to aux eq A(s)0
  • Solution gives imag. axis crossing point -jw
  • System oscillates at frequency w when K is equal
    to the value above

11
  1. When two branches meet and split, you have
    breakaway points. They are double roots. d(s)0
    and d(s) 0 also. Use this to solve for s and k.

12
  • Departure angle at a complex pole
  • Arrival angle at a complex zero
  • Read the book and learn the derivation
  • Will show example
  • Matlab can construct root locus for you
  • Let num n1(s)s coeff vector
  • Let den d1(s)s coeff vector
  • rlocus(num,den) draws locus for the root locus
    equation
  • But you need to first get to Kn1(s)/d1(s) 1 0
  • Should be able to do first 7 steps

13

K
  • e.g.
  • c.l. T.F.
  • o.l. zero no finite zeros 3 infinite
    zeroso.l. poles s 0, -2, -6
  • Mark real axis

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  1. Asymptotes n m 3 0 3angles -180º,
    60º, -60º

15

No complex pole/zero, no need to worry about
departure/arrival angles
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  • Char. poly.
  • num s3 , zeros -3
  • den s(s5)(s22s2)(s6) ,
  • poles0, -5,-6,-1j1
  • Asymptotes n m 4
  • angles 45º, 135º

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Two branches coming out of -5 and -6 are heading
to each other, and will and break away. Without
actually calculating, we know the breakaway point
is somewhere between -5 and -6. Since there are
more dominant poles (poles that are closer to the
jw axis), we dont need to be bothered with
computing the actual numbers for the break away
point. Departure angle at p -1j is
angle(-1j3)-angle(-1j0)-angle(-1j5)-angle(-1
j4)pi/2 ans -0.8885 rad -50.9061 deg
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rlocus(1 3, conv(1 2 2 0,1 11 30))
Hand sketch is close but departure angle is
wrong! Also notice how I used conv.
21
  • Example motor control
  • The closed-loop T.F. from ?r to ? is

22
  • What is the open-loop T.F.?
  • The o.l. T.F. of the system is
  • But for root locus, it depends on which parameter
    we are varying.
  • If KP varies, KD fixed, from char. poly.

23
  • The o.l. T.F. for KP-root-locus is the system
    o.l. T.F.
  • In general, this is the case whenever the
    parameter is in the forward loop.
  • If KD is para, KP is fixedFrom

24
  • More examples
  • No finite zeros, o.l. poles 0,-1,-2
  • Real axis are on R.L.
  • Asymp 3

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  • -axis crossing
  • char. poly

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  • Example
  • Real axis
  • (-2,0) seg. is on R.L.

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  • For

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  • Break away point

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  • -axis crossing
  • char. poly

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  • Example in prev. ex., change s2 to s3

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  • -axis crossing
  • char. poly
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