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    ROOT-LOCUS METHOD

    4 Root-Locus Method

    4.1 Root-Locus Analysis

    (cf. Chapter 6 of the textbook)

    Feedback System:

    +

    KG(s)

    R YE

    where K >0 and

    G(s) = b(s)

    a(s)

    =

    mi=1(s zi)

    n

    i=1(s pi)

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    ROOT-LOCUS METHOD

    Example 4.1 Find a graphical representation

    of all closed-loop poles with respect toK when

    G(s) = 1

    s(s + 1)

    Solution.As the closed-loop transfer function is

    K

    s2 + s + K

    the closed-loop poles can be found to be

    p1, p2= 12 1 4K

    2

    As K varies from 0 to, the two poles forma cross as shown in the following figure.

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    ROOT-LOCUS METHOD

    Re(s)0

    Im(s)

    1

    1

    1

    Definition:The graph of all possible closed-loop poles rel-

    ative to some particular system parameter is

    called the root locus.

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    ROOT-LOCUS METHOD

    Angle and Magnitude Conditions:

    For a given K, a complex number p is a closed-

    loop pole if and only if it satisfies

    G(p)= 180(2k + 1) (k = 0, 1, 2 )

    |KG(p)|= 1

    Characterization of Root Loci:

    The root-locus consists of all points satisfying

    G(s)= 180(2k + 1) (k = 0, 1, 2 )

    Main Steps for Sketching Root Loci:

    Step 1 Mark the open-loop poles with and zeros

    with in the s-plane.

    Step 2 Find the real axis portions of the locus:

    The test point of any real axis portion must

    be to the left of odd number of poles +zeros on the real axis.

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    )1(...,,1,0,360180

    mnk

    mn

    kk

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    ROOT-LOCUS METHOD

    q is the multiplicity of pj or zj, and k is

    chosen so that

    |

    dep| 180 and

    |arr

    | 180

    Remark 4.1 Every branch of a root locus always

    starts at an open-loop pole and ends at an open-

    loop zero or infinity.

    Remark 4.2 A root locus is symmetric about the

    real axis.

    Remark 4.3 The points where the locus crosses

    the imaginary axis can be found by solving

    a(j) + Kb(j) = 0

    Remark 4.4 The locations of multiple closed-loop

    poles on the real axis can be determined by solving

    a(s) + Kb(s) = 0a(s) + Kb(s) = 0

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    ROOT-LOCUS METHOD

    Example 4.2 For

    G(s) =

    1

    s(s + 1)(s + 2)

    sketch the root-locus plot and then determine the

    value of K such that the damping ratio of a pair

    of complex-conjugate closed-loop poles is 0.5.

    Solution.

    To find the breakaway point, we solve

    s(s + 1)(s + 2 ) + K= 0

    [s(s + 1)(s + 2 ) + K] = 0

    The two solutions are

    s= 0.4226 and s= 1.5774The breakaway point is seen to be s = 0.4226 as

    it is between 0 and1.

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    ROOT-LOCUS METHOD

    Example 4.3 For

    G(s) = s + 2s2 + 2s + 3

    sketch the root-locus plot.

    Solution.

    To find the breakin point, we solve

    s2 + 2s + 3 + K(s + 2) = 0

    [s2 + 2s + 3 + K(s + 2)]= 0

    The two solutions are

    s= 3.7320 and s= 0.2680The breakin point is seen to be s =3.7320 asthe other point is not on the root locus.

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    ROOT-LOCUS METHOD

    4.2 Root-Locus Synthesis

    (cf. Chapter 7 of the textbook)

    Dominant Poles: A pair of complex conjugatepoles is said to be dominant if all the other

    poles are to the left of the pair.

    Lead compensators: A lead compensator is asystem whose steady-state response to any si-

    nusoidal input has a phase lead. A first order

    lead compensator is of the form

    C(s) =Ks + b

    s + a, a > b >0

    Lag Compensators: A lead compensator is asystem whose steady-state response to any si-

    nusoidal input has a phase lag. A first order

    lag compensator is of the form

    C(s) =Ks + bs + a

    , 0< a < b

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    ROOT-LOCUS METHOD

    Lag-Lead Compensators: A lag-lead compen-sator is a system whose steady-state response

    to a sinusoidal input has a phase lag in some

    frequency region and a phase lead in another.

    Role of Compensation: A compensator is tocompensate for deficit performance of the orig-

    inal system.

    Realization of Compensators: electronic net-works and mechanical systems.

    +u

    +y

    R1

    R2

    C

    Lead network.

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    ROOT-LOCUS METHOD

    +

    u

    +

    y

    R1

    R2

    C

    Lag network.

    Compensation technique:Consider the following feedback system dia-

    gram:

    +

    C(s) P(s)

    R Y

    Feedback control system.

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    ROOT-LOCUS METHOD

    whereP(s) is the transfer function of the plant

    to be controlled and C(s) is a first-order com-

    pensator of the form

    C(s) =Ks + b

    s + a

    As the open-loop transfer function isP(s)C(s),

    the angle and magnitude conditions for the

    root locus are

    P(s)C(s) = 180(2k+ 1) (k= 0, 1, 2 )|P(s)C(s)| = 1

    i.e.

    [(s + b)(s + a)] + P(s) =

    180

    (2k+ 1)

    |C(s)||P(s)| = 1The basic compensation technique consists of

    two steps:

    Determine the location of the pole and zero

    of C(S) from the angle condition.

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    ROOT-LOCUS METHOD

    Compute the gain of C(s) from the magni-

    tude condition.

    The complete procedure for designing a com-pensator:

    Step 1 Determine the desired location for the dom-

    inant closed-loop poles from the performance

    specifications.

    Step 2 Ascertain whether or not the gain adjust-

    ment alone can yield the desired closed-loop

    poles by e.g. drawing the root-locus plot.

    If not, go to the next step.

    Step 3 If not, determine the angle contribution of

    the compensator from the angle of P(s) at

    a dominant closed-loop pole.

    Step 4 Determine the location of the pole and zeroof the compensator.

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    ROOT-LOCUS METHOD

    Step 5 Determine the gain of the compensator from

    the magnitude condition.

    Step 6 Verify that all performance specifications have

    been met.

    Example 4.4 Consider the system shown as

    on page 88, where

    P(s)=4

    s(s+ 2)

    Design a lead compensator C(s) so that the

    closed-loop system has poles at

    jp 322

    and has a static velocity error as small aspos-

    sible.

    Solution.

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    ROOT-LOCUS METHOD

    Step 1 Note from the root-locus plot shown below

    that a proportional controller cannot place

    the closed-loop poles at the desired loca-

    tion.

    Re(s)0

    Im(s)

    2

    2

    2

    Step 2 As the angle of P(s) at p= 2 + 23j is

    4

    s(s + 2)

    s=2+23j

    = 210o

    the angle condition will be satisfied whenthe angle contribution of the compensator

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    ROOT-LOCUS METHOD

    is 30o, i.e.,

    = (p + b) (p + a) = 300 (4.1)

    Step 3 As the static velocity error constant of the

    closed-loop system is

    Kv =K(b/a) lims0 sP(s) (4.2)

    a and b should be chosen so that (4.1) is

    satisfied and b/a is maximized. The follow-

    ing figure explains how to calculate such apair which is given by

    a= 5.4 and b= 2.9

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    ROOT-LOCUS METHOD

    Re

    Im

    0

    p

    b

    a

    2

    2

    Step 4 From the magnitude condition, the gain of

    the compensator is found to be

    K= 4.68

    It follows from (4.2) that the static velocity

    error constant is

    Kv = 5.02

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    ROOT-LOCUS METHOD

    Step 5 The resulting closed-loop poles are

    p= 2 2

    3j and 3.4The following figure exhibits the unit-step

    and unit-ramp responses of the closed-loop

    systems associated with

    C(s) = 1 and C(s) = 4.68s + 2.9

    s + 5.4

    respectively.

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    ROOT-LOCUS METHOD

    0 0.5 1 1.5 2 2.5 3 3.5 40

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    1.4UnitStep Responses of Compensated and Uncompensated Systems

    t Sec

    Output

    Compensated System

    Uncompensated System

    Unit-step responses of compensated and

    uncompensated systems.

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    ROOT-LOCUS METHOD

    0 0.5 1 1.5 2 2.5 3 3.5 40

    0.5

    1

    1.5

    2

    2.5

    3

    3.5

    4UnitRamp Responses of Compensated and Uncompensated Systems

    t Sec

    Output

    Uncompensated System

    Compensated System

    UnitRamp Input

    Unit-ramp responses of compensated and

    uncompensated systems.

    97