Question 3 of 6: Routh Stability Range and Root Locus for System 1.0
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 07-Mec-A3 System Analysis and Control, National Exams May 2016 — 3 hours, closed book (Casio or Sharp approved calculator; semi-log graph paper is the only permitted aid). The rubric states that any four (4) questions constitute a complete paper and that all questions are of equal value, so each question is worth 25 marks of the 100 marked. Because this document is a study resource rather than an exam script, all six questions are solved in full.
Reference texts. K. Ogata, Modern Control Engineering, 5th ed. (Pearson) — Ch. 3–7; N. S. Nise, Control Systems Engineering, 8th ed. (Wiley) — Ch. 4, 6, 8, 10; R. C. Dorf and R. H. Bishop, Modern Control Systems, 13th ed. (Pearson) — Ch. 5–8; G. F. Franklin, J. D. Powell and A. Emami-Naeini, Feedback Control of Dynamic Systems, 8th ed. (Pearson) — Ch. 3–6. A table of Laplace transform pairs is appended to the examination paper (pages 3–4 of the original), together with two sheets of 3-cycle semi-logarithmic graph paper for the Bode question.
Question 3: Routh Stability Range and Root Locus for System 1.0 (25 marks)
Given. The block diagram of System 1.0 (reproduced below from page 2 of the paper):
[Figure not reproduced: Figure 3.1 — System 1.0 as printed on the examination paper: forward path $K\,(s+3)/[s(s^{2}+4s+5)]$, negative feedback through $1/(s+1)$. See the official exam paper.]
Find. (a) the complete range of $K$ giving a stable closed loop, by the Routh–Hurwitz criterion; (b) the root locus versus $K$, annotated with departure and arrival angles, the breakaway and break-in points with their gains, and the imaginary-axis crossings with their gain and frequency.
Approach. Form the characteristic polynomial $1+L(s)=0$, build the Routh array symbolically in $K$ and require every first-column entry to be positive; then construct the locus from the standard rules (real-axis segments, asymptote centroid and angles, $dK/ds=0$ for breakaway/break-in, the angle criterion for departure, and the Routh auxiliary polynomial for the axis crossing).
Part (a) — Routh–Hurwitz
Form the characteristic polynomial. Setting $1+L(s)=0$ and clearing denominators,$$s(s+1)(s^{2}+4s+5)+K(s+3)=0$$Expanding the product $s(s+1)(s^{2}+4s+5)=(s^{2}+s)(s^{2}+4s+5)=s^{4}+5s^{3}+9s^{2}+5s$ gives$$\Delta(s)=s^{4}+5s^{3}+9s^{2}+(5+K)s+3K=0$$A necessary condition is immediate: every coefficient must be positive, so $K>0$ at the very least.
Build the Routh array in terms of $K$.$$\begin{array}{c|ccc}s^{4}&1&9&3K\\ s^{3}&5&5+K&0\\ s^{2}&b_{1}&3K&\\ s^{1}&c_{1}&&\\ s^{0}&3K&&\end{array}$$with$$b_{1}=\frac{5(9)-1(5+K)}{5}=\frac{40-K}{5},\qquad c_{1}=\frac{b_{1}(5+K)-5(3K)}{b_{1}}=(5+K)-\frac{75K}{40-K}$$
Impose positivity of the whole first column. The $s^{0}$ row requires $3K>0$, i.e. $K>0$. The $s^{2}$ row requires $40-K>0$. The binding condition is the $s^{1}$ row; multiplying through by the positive quantity $(40-K)$,$$(5+K)(40-K)-75K>0\;\Longrightarrow\;200+35K-K^{2}-75K>0\;\Longrightarrow\;K^{2}+40K-200<0$$The positive root of $K^{2}+40K-200=0$ is$$K_{\max}=\frac{-40+\sqrt{1600+800}}{2}=\frac{-40+20\sqrt{6}}{2}=-20+10\sqrt6$$
Collect the range. Since $-20+10\sqrt6=4.4949<40$, the $s^{2}$ condition is not binding and the answer is$$\boxed{\;0<K<-20+10\sqrt6=4.495\;}$$A numerical spot check confirms it: at $K=4$ the closed-loop roots are all in the left half-plane, while at $K=5$ a conjugate pair has crossed into the right half-plane.
Part (b) — Root locus
Identify the open-loop poles and zeros. From $L(s)=K(s+3)/[s(s+1)(s^{2}+4s+5)]$ the four poles are $s=0,\;-1,\;-2\pm j1$ (since $s^{2}+4s+5=(s+2)^{2}+1$) and the single finite zero is $s=-3$. Hence $n=4$, $m=1$ and $n-m=3$ branches go to infinity.
Real-axis segments. A point on the real axis belongs to the $K>0$ locus when the number of real poles and zeros to its right is odd. Counting from the right: the interval $(-1,\,0)$ has one (the pole at the origin) and is on the locus; $(-3,\,-1)$ has two and is off; $(-\infty,\,-3)$ has three and is on.
Asymptote centroid and angles.$$\sigma_{a}=\frac{\sum p_{i}-\sum z_{j}}{n-m}=\frac{\bigl(0-1-2-2\bigr)-(-3)}{3}=\frac{-5+3}{3}=-\frac{2}{3}=-0.667$$$$\theta_{a}=\frac{(2k+1)180^{\circ}}{3}=60^{\circ},\;180^{\circ},\;300^{\circ}$$
Angle of departure from the complex poles. The angle criterion at $s_{0}=-2+j1$ gives$$\theta_{d}=180^{\circ}+\sum\angle(s_{0}-z_{j})-\sum_{i\neq0}\angle(s_{0}-p_{i})$$With $\angle(s_{0}+3)=\angle(1+j1)=45^{\circ}$ and the pole contributions $\angle(s_{0}-0)=153.43^{\circ}$, $\angle(s_{0}+1)=135^{\circ}$, $\angle(s_{0}+2+j1)=\angle(j2)=90^{\circ}$,$$\theta_{d}=180^{\circ}+45^{\circ}-\left(153.43^{\circ}+135^{\circ}+90^{\circ}\right)=-153.43^{\circ}$$so$$\boxed{\;\theta_{d}=-153.4^{\circ}\text{ at }s=-2+j1,\qquad +153.4^{\circ}\text{ at }s=-2-j1\;}$$The branch therefore leaves the complex pole heading down and to the left, consistent with the sketch below.
Angle of arrival at the finite zero. Applying the mirror-image criterion at $s=-3$, the four pole vectors contribute $180^{\circ}+180^{\circ}+(-135^{\circ})+135^{\circ}=360^{\circ}$, so$$\theta_{a,\,z}=180^{\circ}+360^{\circ}\equiv180^{\circ}$$i.e. the branch arrives at the zero along the real axis from the left, as it must, since $-3$ is the right-hand end of the real-axis segment $(-\infty,-3)$.
Breakaway and break-in points. Writing $K(s)=-\dfrac{s(s+1)(s^{2}+4s+5)}{s+3}$ and solving $dK/ds=0$ yields four roots; only the two real ones lying on $K>0$ segments are physical:$$s_{b}=-0.4363\;\text{(in }(-1,0)\text{)}\quad\text{and}\quad s_{r}=-3.6503\;\text{(in }(-\infty,-3)\text{)}$$Substituting each back into $K(s)$,$$\boxed{\;\text{breakaway: }s=-0.436,\;K=0.331\qquad\text{break-in: }s=-3.650,\;K=55.39\;}$$The remaining pair of $dK/ds=0$ roots, $s=-1.623\pm j0.710$, returns a complex gain and therefore belongs to no real-$K$ locus at all — it is discarded.
Imaginary-axis crossings. At $K=K_{\max}$ the $s^{1}$ row vanishes and the auxiliary polynomial from the $s^{2}$ row gives the crossing frequency:$$\frac{40-K}{5}\,s^{2}+3K=0\;\Longrightarrow\;s^{2}=-\frac{15K}{40-K}$$At $K=4.4949$ this is $s^{2}=-1.8990$, so$$\boxed{\;s=\pm j1.378\ \text{rad/s at }K=4.495\;}$$Solving the quartic at that gain confirms the picture: the roots are $\pm j1.378$ together with a well-damped pair at $-2.500\pm j0.923$.
Figure 3.2 — Root locus of $1+K(s+3)/[s(s+1)(s^{2}+4s+5)]=0$ for $K>0$. Crosses are open-loop poles, the circle is the zero at $s=-3$. Two branches leave the poles at $0$ and $-1$, break away at $s=-0.436$ ($K=0.331$) and cross the imaginary axis at $\pm j1.378$ when $K=4.495$; the branches from $-2\pm j1$ depart at $\mp153.4^{\circ}$, meet the real axis at the break-in point $s=-3.650$ ($K=55.39$), and thereafter one runs to the zero at $-3$ while the other escapes along the $180^{\circ}$ asymptote.
The locus and the Routh result agree exactly, which is the intended cross-check of the question: the gain at which the branches pierce the imaginary axis is precisely the $K_{\max}$ delivered by the $s^{1}$ row, and the frequency of that crossing is precisely the root of the auxiliary polynomial. Note also the qualitative message — the loop is stable only over a rather narrow band of gain, and the limit is imposed not by the plant alone but by the extra lag $1/(s+1)$ in the measurement path, which contributes an additional $90^{\circ}$ of phase at high frequency.