Skip to main content

Root locus of K/[s(s²+10s+24)] at ζ = 0.7

Short answer

For damping ratio 0.7, the closed-loop poles are at -1.39±j1.42, found by solving the angle condition along the ζ=0.7 line. Using the magnitude condition, gain K≈28.4 and natural frequency ωn≈1.98 rad/s.

Draw the root locus for the system with open loop transfer function as G(s)H(s) = K/[s(s²+10s+24)] and hence from the root locus, find the gain (K) and corresponding natural frequency of oscillation when the damping ratio is 0.7.

Result: at ζ=0.7\zeta=0.7, K≈28.4K \approx 28.4, with ωn≈1.98\omega_n \approx 1.98 rad/s and ωd≈1.42\omega_d \approx 1.42 rad/s.

The root locus is sketched with the standard rules. The ζ=0.7\zeta = 0.7 line is then drawn from the origin, and the magnitude condition at its intersection with the locus gives KK.

G(s)H(s)=Ks(s2+10s+24)=Ks(s+4)(s+6)G(s)H(s) = \frac{K}{s(s^2+10s+24)} = \frac{K}{s(s+4)(s+6)}

Step 1: Poles and zeros

Poles: 0, −4, −60,\ -4,\ -6 (n=3n=3). No zeros (m=0m=0), so 3 branches go to infinity.

Step 2: Real-axis segments

Between 00 and −4-4, and from −6-6 to −∞-\infty.

Step 3: Asymptotes

θ=(2q+1)180∘3=60∘, 180∘, 300∘,σA=0−4−63=−3.33\theta = \frac{(2q+1)180^\circ}{3} = 60^\circ,\ 180^\circ,\ 300^\circ, \qquad \sigma_A = \frac{0-4-6}{3} = -3.33

Step 4: Breakaway point

K=−(s3+10s2+24s)dKds=−(3s2+20s+24)=0s=−20±400−2886=−1.57 or −5.10\begin{aligned} K &= -(s^3+10s^2+24s) \\ \frac{dK}{ds} &= -(3s^2+20s+24) = 0 \\ s &= \frac{-20\pm\sqrt{400-288}}{6} = -1.57 \ \text{or}\ -5.10 \end{aligned}

s=−5.10s=-5.10 is not on the locus. So the breakaway point is s=−1.57s=-1.57, where K=∣s∣∣s+4∣∣s+6∣=16.9K = |s||s+4||s+6| = 16.9.

Step 5: Imaginary-axis crossing

Characteristic equation: s3+10s2+24s+K=0s^3+10s^2+24s+K=0

RowCol 1Col 2
s3s^3124
s2s^210KK
s1s^1240−K10\frac{240-K}{10}
s0s^0KK

K=240K = 240 makes the s1s^1 row zero, and 10s2+240=010s^2+240=0 gives s=±j4.90s = \pm j4.90. The system is stable for 0<K<2400<K<240.

Step 6: Point with ζ=0.7\zeta = 0.7

The constant-ζ\zeta line makes angle θ=cos⁡−10.7=45.57∘\theta = \cos^{-1}0.7 = 45.57^\circ with the negative real axis. Points on it are s=−0.7ωn+j0.714ωns = -0.7\omega_n + j0.714\omega_n. Using the angle condition ∠s+∠(s+4)+∠(s+6)=180∘\angle s + \angle(s+4) + \angle(s+6) = 180^\circ (solved by trial):

ωn=1.984 rad/s,s=−1.389±j1.417\omega_n = 1.984\ \text{rad/s}, \qquad s = -1.389 \pm j1.417

Magnitude condition:

K=∣s∣ ∣s+4∣ ∣s+6∣=1.984×2.971×4.824=28.4K = |s|\,|s+4|\,|s+6| = 1.984 \times 2.971 \times 4.824 = 28.4

The third closed-loop pole is then at s≈−7.22s \approx -7.22, far to the left, so the complex pair is dominant.

Sketch

 Upper half shown; lower half is its mirror image.

                            jw      /
                             |     / 60 deg asymptote
                             *    /  (from -3.33)
                            /| j4.90 (K=240)
                           / |
                          /  |
     zeta=0.7 point -->  *   |  -1.39+j1.42 (K=28.4)
                         |.  |
                         | . |   . = zeta line
                         |  .|
  <====x------x==========o===x----> sigma
      -6     -4       -1.57  0
                     (K=16.9)

Answer: at ζ=0.7\zeta = 0.7: K≈28.4K \approx 28.4, natural frequency ωn≈1.98\omega_n \approx 1.98 rad/s (damped frequency ωd=ωn1−ζ2≈1.42\omega_d = \omega_n\sqrt{1-\zeta^2} \approx 1.42 rad/s). Closed-loop dominant poles are at −1.39±j1.42-1.39 \pm j1.42.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Control Systems chapter 5 questions →