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Root locus of K/[s(s+1)(s²+4s+5)], critical damping

Draw root locus for unity feedback system with feedforward transfer function G(s) = K/[s(s+1)(s²+4s+5)]. Also, clearly identify the value of K for critical damping of the system.

The root locus is the path of the closed-loop poles in the s-plane as KK varies from 0 to ∞\infty. The characteristic equation is 1+G(s)=01 + G(s) = 0, i.e.

s(s+1)(s2+4s+5)+K=0  ⇒  s4+5s3+9s2+5s+K=0s(s+1)(s^2+4s+5) + K = 0 \;\Rightarrow\; s^4 + 5s^3 + 9s^2 + 5s + K = 0

Step 1: Poles, zeros and branches

  • Open-loop poles: s=0, −1, −2±j1s = 0,\ -1,\ -2 \pm j1 (n=4n = 4); zeros: none (m=0m = 0).
  • Number of branches = 4; all four go to infinity.

Step 2: Real-axis locus

A real-axis point is on the locus if the number of real poles + zeros to its right is odd. Only the segment between 0 and −1 qualifies.

Step 3: Asymptotes

σA=∑p−∑zn−m=0−1−2−24=−1.25θA=(2q+1)180∘4=±45∘, ±135∘\begin{aligned} \sigma_A &= \frac{\sum p - \sum z}{n-m} = \frac{0-1-2-2}{4} = -1.25 \\ \theta_A &= \frac{(2q+1)180^\circ}{4} = \pm 45^\circ,\ \pm 135^\circ \end{aligned}

Step 4: Breakaway point

K=−(s4+5s3+9s2+5s)K = -(s^4+5s^3+9s^2+5s), so

dKds=−(4s3+15s2+18s+5)=0\frac{dK}{ds} = -(4s^3+15s^2+18s+5) = 0

Roots: s=−0.393s = -0.393 and s=−1.679±j0.603s = -1.679 \pm j0.603. Only s=−0.393s = -0.393 lies on the locus (between 0 and −1). Gain there:

K=0.393×0.607×∣(−0.393)2+4(−0.393)+5∣=0.855K = 0.393 \times 0.607 \times |(-0.393)^2 + 4(-0.393) + 5| = 0.855

Step 5: Angle of departure from −2+j1-2+j1

Angles from the other poles to −2+j1-2+j1: from 00: 153.43∘153.43^\circ; from −1-1: 135∘135^\circ; from −2−j1-2-j1: 90∘90^\circ.

ϕd=180∘−(153.43∘+135∘+90∘)=−198.43∘≡161.57∘\phi_d = 180^\circ - (153.43^\circ + 135^\circ + 90^\circ) = -198.43^\circ \equiv 161.57^\circ

By symmetry, the angle from −2−j1-2-j1 is −161.57∘-161.57^\circ.

Step 6: Imaginary-axis crossing (Routh array)

RowCol 1Col 2Col 3
s4s^419KK
s3s^355
s2s^28KK
s1s^1(40−5K)/8(40-5K)/8
s0s^0KK

Marginal stability: 40−5K=0⇒K=840 - 5K = 0 \Rightarrow K = 8. Auxiliary equation: 8s2+8=0⇒s=±j18s^2 + 8 = 0 \Rightarrow s = \pm j1. The locus crosses the jωj\omega axis at ±j1\pm j1 rad/s when K=8K = 8.

Sketch

                                    |
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    ...                             |       ..
      .....                         |    ....
          ....                      | ....
             .....x                .X..
                                 ...|
                                ..  |
---------------------------x....*...x-------------
                                ..  |
                                 ...|
             .....x                .X..
          ....                      | ....
      .....                         |    ....
    ...                             |       ..
                                    |
                                    |
                 -2       -1        0
x pole   * breakaway (-0.393)
X jw crossing (+-j1, K = 8)

Branches from 0 and −1 meet at −0.393, break away at ±90°, and bend toward the ±45° asymptotes, crossing at ±j1 (K = 8). Branches from −2±j1-2\pm j1 leave at ±161.6∘\pm 161.6^\circ and approach the ±135° asymptotes.

Gain for critical damping

Critical damping occurs when the dominant closed-loop poles are real and equal, i.e. at the breakaway point s=−0.393s = -0.393. The other two poles are then at −2.107±j1.046-2.107 \pm j1.046.

Answer: Critical damping at K ≈ 0.855 (double pole at s = −0.393). The system is stable for 0<K<80 < K < 8.

✓ Answer checked by Claude Opus 5.5 (high effort)

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