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Root locus of k/[s(s+4)(s²+4s+20)]

Short answer

Breakaway points are at s=-2 (K=64) and s=-2±j2.45 (K=100). The departure angle from -2+j4 is -90° (and +90° from -2-j4). The system is stable for 0<K<260, marginally stable at K=260 with crossing at ±j3.16, and unstable for K>260.

For a unity feedback system the open loop transfer function of a control system is given by G(s) = k/[s(s+4)(s²+4s+20)]. Sketch the root locus for 0 ≤ K ≤ ∞ and determine the breakaway point, the angle of departure from complex poles and the stability conditions.

The root locus is the path traced by the closed-loop poles (roots of 1+G(s)H(s)=01+G(s)H(s)=0) as KK varies from 0 to ∞\infty. It is sketched using the standard construction rules.

G(s)H(s)=Ks(s+4)(s2+4s+20)G(s)H(s) = \frac{K}{s(s+4)(s^2+4s+20)}

Step 1: Poles and zeros

  • Poles: s=0s=0, s=−4s=-4, s=−2±j4s=-2\pm j4 (from s2+4s+20=0s^2+4s+20=0). So n=4n=4.
  • Zeros: none, m=0m=0. All 4 branches go to infinity.

Step 2: Real-axis locus

A point on the real axis is on the locus if the number of poles + zeros to its right is odd. So the locus lies between 00 and −4-4.

Step 3: Asymptotes

θq=(2q+1)180∘n−m=45∘, 135∘, 225∘, 315∘σA=∑poles−∑zerosn−m=0−4−2−24=−2\begin{aligned} \theta_q &= \frac{(2q+1)180^\circ}{n-m} = 45^\circ,\ 135^\circ,\ 225^\circ,\ 315^\circ \\ \sigma_A &= \frac{\sum \text{poles} - \sum\text{zeros}}{n-m} = \frac{0-4-2-2}{4} = -2 \end{aligned}

Step 4: Breakaway points

K=−s(s+4)(s2+4s+20)=−(s4+8s3+36s2+80s)dKds=−(4s3+24s2+72s+80)=0⇒s3+6s2+18s+20=0⇒(s+2)(s2+4s+10)=0s=−2,s=−2±j2.45\begin{aligned} K &= -s(s+4)(s^2+4s+20) = -(s^4+8s^3+36s^2+80s) \\ \frac{dK}{ds} &= -(4s^3+24s^2+72s+80) = 0 \\ &\Rightarrow s^3 + 6s^2 + 18s + 20 = 0 \\ &\Rightarrow (s+2)(s^2+4s+10) = 0 \\ s &= -2,\quad s = -2\pm j2.45 \end{aligned}
  • At s=−2s=-2: K=−(16−64+144−160)=64>0K = -(16-64+144-160) = 64 > 0, a valid breakaway point (on the real-axis segment).
  • At s=−2±j2.45s=-2\pm j2.45: K=100K = 100 (real and positive), so these are also valid break points.

So the branches from 00 and −4-4 meet at −2-2 (K=64K=64) and leave vertically along s=−2s=-2. They meet the branches coming down from −2±j4-2\pm j4 at −2±j2.45-2\pm j2.45 (K=100K=100). Then they break away again towards the 45∘45^\circ and 135∘135^\circ asymptotes.

Step 5: Angle of departure from complex pole −2+j4-2+j4

Angles from the other poles to −2+j4-2+j4:

  • From s=0s=0: 180∘−tan⁡−1(4/2)=116.57∘180^\circ - \tan^{-1}(4/2) = 116.57^\circ
  • From s=−4s=-4: tan⁡−1(4/2)=63.43∘\tan^{-1}(4/2) = 63.43^\circ
  • From s=−2−j4s=-2-j4: 90∘90^\circ
ϕd=180∘−(116.57∘+63.43∘+90∘)=−90∘\phi_d = 180^\circ - (116.57^\circ + 63.43^\circ + 90^\circ) = -90^\circ

So the locus leaves −2+j4-2+j4 straight downwards (−90∘-90^\circ), and leaves −2−j4-2-j4 at +90∘+90^\circ.

Step 6: Crossing of the imaginary axis (Routh)

Characteristic equation: s4+8s3+36s2+80s+K=0s^4+8s^3+36s^2+80s+K=0

RowCol 1Col 2Col 3
s4s^4136KK
s3s^3880
s2s^28(36)−808=26\frac{8(36)-80}{8}=26KK
s1s^126(80)−8K26\frac{26(80)-8K}{26}
s0s^0KK

s1s^1 row =0=0: 2080−8K=0⇒K=2602080 - 8K = 0 \Rightarrow K = 260. Auxiliary equation: 26s2+260=0⇒s=±j3.1626s^2 + 260 = 0 \Rightarrow s = \pm j3.16.

Step 7: Sketch

 Upper half shown; lower half is its mirror image.

  \                          jw        /
   \  135 deg asymptote      |        /  45 deg
    \                        |       /   asymptote
     \__                     * j3.16 (K=260)
        \      x -2+j4     _/|
         \__   |         _/  |
            \  v       _/    |
             `-o------'      |
         -2+j2.45 (K=100)    |
               ^             |
               |             |
   ----x=======o=============x---- sigma
      -4      -2 (K=64)      0

Results

ItemValue
Breakaway pointss=−2s=-2 (K=64K=64); s=−2±j2.45s=-2\pm j2.45 (K=100K=100)
Angle of departure−90∘-90^\circ at −2+j4-2+j4, +90∘+90^\circ at −2−j4-2-j4
jωj\omega crossings=±j3.16s=\pm j3.16 at K=260K=260
StabilityStable for 0<K<2600<K<260; marginally stable at K=260K=260; unstable for K>260K>260

✓ Answer checked by Claude Opus 5.5 (high effort)

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