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Root locus criteria; poles 0, −1±j2

Short answer

Root locus uses angle criterion (sum of zero angles minus pole angles = odd multiple of 180°) and magnitude criterion (|GH|=1 to find K). For poles at 0, -1±j2, G(s)=K/[s(s²+2s+5)]. System stable for 0<K<10; at K=10 it oscillates at 2.236 rad/s.

Mention the criteria of Root locus plot. Write open loop transfer function and hence sketch the root locus of unity feedback system whose open loop poles and zeros are as shown in s plane below. [Figure: s-plane with open-loop poles at s = 0 and s = −1 ± j2; no zeros shown]

Criteria of root locus

Every point ss on the root locus satisfies the characteristic equation 1+G(s)H(s)=01 + G(s)H(s) = 0, i.e. G(s)H(s)=−1G(s)H(s) = -1. This gives two conditions:

  1. Angle criterion: ∠G(s)H(s)=±(2q+1)180∘\angle G(s)H(s) = \pm(2q+1)180^\circ, q=0,1,2,…q = 0, 1, 2, \dots The sum of angles from the zeros minus the sum of angles from the poles must be an odd multiple of 180∘180^\circ. A point is on the locus only if it meets this condition.
  2. Magnitude criterion: ∣G(s)H(s)∣=1|G(s)H(s)| = 1. This gives the value of KK at a point already known to be on the locus:
K=∏∣s−pi∣∏∣s−zj∣K = \frac{\prod |s - p_i|}{\prod |s - z_j|}

Open-loop transfer function

Poles at 00 and −1±j2-1 \pm j2, no zeros:

G(s)=Ks[(s+1)2+4]=Ks(s2+2s+5)G(s) = \frac{K}{s\left[(s+1)^2 + 4\right]} = \frac{K}{s(s^2+2s+5)}

Characteristic equation: s3+2s2+5s+K=0s^3 + 2s^2 + 5s + K = 0.

Sketching steps

  1. Branches: n=3n = 3, m=0m = 0, so there are 3 branches and all go to infinity.
  2. Real-axis locus: the whole negative real axis, from 00 to −∞-\infty (one pole to the right).
  3. Asymptotes:
σA=0−1−13=−0.667,θA=60∘, 180∘, 300∘\sigma_A = \frac{0 - 1 - 1}{3} = -0.667, \qquad \theta_A = 60^\circ,\ 180^\circ,\ 300^\circ
  1. Breakaway: dK/ds=−(3s2+4s+5)=0⇒s=−0.667±j1.106dK/ds = -(3s^2 + 4s + 5) = 0 \Rightarrow s = -0.667 \pm j1.106. These are complex, so there is no breakaway point. The branch from the origin moves straight along the negative real axis to −∞-\infty.
  2. Angle of departure from −1+j2-1 + j2: from pole 00: 116.57∘116.57^\circ; from −1−j2-1-j2: 90∘90^\circ.
ϕd=180∘−(116.57∘+90∘)=−26.57∘\phi_d = 180^\circ - (116.57^\circ + 90^\circ) = -26.57^\circ

At −1−j2-1-j2, it is +26.57∘+26.57^\circ. 6. jωj\omega-axis crossing (Routh):

RowCol 1Col 2
s3s^315
s2s^22KK
s1s^1(10−K)/2(10-K)/2
s0s^0KK

Kmar=10K_{mar} = 10; auxiliary equation 2s2+10=0⇒s=±j5=±j2.2362s^2 + 10 = 0 \Rightarrow s = \pm j\sqrt5 = \pm j2.236.

Sketch

                                    |         ....
                                    |      ....
                                    |   ....
                                    .....
                           x........X
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....................................x-------------
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                           x........X
                                    .....
                                    |   ....
                                    |      ....
                                    |         ....
        -3                -1        0
x pole (0, -1 +- j2)
X jw crossing (+-j2.24, K = 10)

The complex poles leave at ∓26.6∘\mp 26.6^\circ, bend toward the ±60° asymptotes from −0.667-0.667, and cross the imaginary axis at ±j2.236\pm j2.236.

Answer: G(s)=K/[s(s2+2s+5)]G(s) = K/[s(s^2+2s+5)]; stable for 0<K<100 < K < 10; at K=10K = 10 it oscillates at ω=2.236\omega = 2.236 rad/s.

✓ Answer checked by Claude Opus 5.5 (high effort)

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