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Root locus of K(s+1)/[(s²+2s+2)(s²+2s+5)]

Short answer

Poles at -1±j1 and -1±j2, zero at -1. Real-axis locus extends left of -1. Asymptotes are 60°,180°,300° from σ=-1. Departure angles are 180° from -1±j1 and 0° from -1±j2. Break-in at s=-1.77 (k=9.5). Imaginary-axis crossing at ±j2.74 (k=16.12), stable for 0<k<16.12.

Sketch Root locus plot for the system having open loop transfer function G(s)H(s) = k(s+1)/[(s²+2s+2)(s²+2s+5)].

The root locus is drawn for 0≤k<∞0 \le k < \infty with the standard construction rules.

G(s)H(s)=k(s+1)(s2+2s+2)(s2+2s+5)G(s)H(s) = \frac{k(s+1)}{(s^2+2s+2)(s^2+2s+5)}

Step 1: Poles and zeros

  • Poles: s=−1±j1s = -1\pm j1 and s=−1±j2s = -1 \pm j2, so n=4n = 4.
  • Zero: s=−1s = -1, so m=1m = 1.
  • Number of branches = 4. One branch ends at the zero and three go to infinity.

Step 2: Real-axis locus

There are no real poles. The only real-axis singularity is the zero at −1-1. Points to the left of −1-1 have one zero to their right (odd), so the real axis from −1-1 to −∞-\infty is on the locus.

Step 3: Asymptotes

θq=(2q+1)180∘n−m=60∘, 180∘, 300∘σA=(−1−1−1−1)−(−1)3=−33=−1\begin{aligned} \theta_q &= \frac{(2q+1)180^\circ}{n-m} = 60^\circ,\ 180^\circ,\ 300^\circ \\ \sigma_A &= \frac{(-1-1-1-1)-(-1)}{3} = \frac{-3}{3} = -1 \end{aligned}

Step 4: Angles of departure

At p1=−1+j1p_1 = -1+j1, angles from the other poles and the zero:

  • from −1−j1-1-j1: 90∘90^\circ; from −1+j2-1+j2: −90∘-90^\circ; from −1−j2-1-j2: 90∘90^\circ
  • from zero −1-1: 90∘90^\circ
ϕd1=180∘−(90∘−90∘+90∘)+90∘=180∘\phi_{d1} = 180^\circ - (90^\circ - 90^\circ + 90^\circ) + 90^\circ = 180^\circ

At p2=−1+j2p_2 = -1+j2:

  • from −1+j1-1+j1, −1−j1-1-j1, −1−j2-1-j2: 90∘90^\circ each; from zero: 90∘90^\circ
ϕd2=180∘−270∘+90∘=0∘\phi_{d2} = 180^\circ - 270^\circ + 90^\circ = 0^\circ

So the branch from −1+j1-1+j1 leaves horizontally to the left, and the branch from −1+j2-1+j2 leaves horizontally to the right. The lower half is the mirror image.

Step 5: Break-in point

k=−(s2+2s+2)(s2+2s+5)s+1k = -\frac{(s^2+2s+2)(s^2+2s+5)}{s+1}

Put p=s+1p = s+1, so k=−(p2+1)(p2+4)pk = -\frac{(p^2+1)(p^2+4)}{p}:

dkdp=0⇒3p4+5p2−4=0⇒p2=0.591 (other root negative)\frac{dk}{dp} = 0 \Rightarrow 3p^4 + 5p^2 - 4 = 0 \Rightarrow p^2 = 0.591 \ \text{(other root negative)}

p=−0.769p = -0.769 gives s=−1.77s = -1.77 (on the locus) with k=9.50>0k = 9.50 > 0. So s=−1.77s = -1.77 is a break-in point. The branches from −1±j1-1\pm j1 meet here. After that, one goes right to the zero at −1-1 and the other goes left to −∞-\infty. The roots p=±j1.50p=\pm j1.50 give a complex kk, so they are not on the locus.

Step 6: Imaginary-axis crossing

Characteristic equation: s4+4s3+11s2+(14+k)s+(10+k)=0s^4 + 4s^3 + 11s^2 + (14+k)s + (10+k) = 0

RowCol 1Col 2Col 3
s4s^411110+k10+k
s3s^3414+k14+k
s2s^230−k4\frac{30-k}{4}10+k10+k
s1s^1(30−k)(14+k)−16(10+k)30−k\frac{(30-k)(14+k)-16(10+k)}{30-k}
s0s^010+k10+k

s1s^1 row =0=0: 260−k2=0⇒k=16.12260 - k^2 = 0 \Rightarrow k = 16.12.

Auxiliary equation: 30−16.124s2+26.12=0⇒s=±j2.74\frac{30-16.12}{4}s^2 + 26.12 = 0 \Rightarrow s = \pm j2.74.

Sketch

 Upper half shown; lower half is its mirror image.

                         jw     /
                          |    /  60 deg asymptote
                          *   /   (from -1)
                         /| j2.74 (k=16.1)
              x-------- ' |
            -1+j2  (0 deg)|
                          |
         .--x (180 deg)   |
        /  -1+j1          |
       /                  |
 <====o=====o-------------+-----> sigma
   -1.77   -1             0
  (k=9.5)  zero

Results

ItemValue
Asymptotes60∘,180∘,300∘60^\circ, 180^\circ, 300^\circ from σA=−1\sigma_A=-1
Departure angles180∘180^\circ at −1±j1-1\pm j1; 0∘0^\circ at −1±j2-1\pm j2
Break-in points=−1.77s=-1.77, k=9.5k=9.5
jωj\omega crossing±j2.74\pm j2.74 at k=16.12k=16.12
StabilityStable for 0<k<16.120<k<16.12

✓ Answer checked by Claude Opus 5.5 (high effort)

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