22-Mec-A3 System Analysis and Control · December 2017
Question 2 of 6: Routh Stability — Range of Gain and an Open-Loop Unstable Plant
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2017 — 16-Mec-A3, System Analysis and Control. Three hours, closed book; a Casio or Sharp approved calculator and semi-log graph paper are the only permitted aids. Six questions are printed; any four constitute a complete paper and all questions are of equal value (25 marks each). A table of Laplace transforms is supplied as page 5. All six questions are solved here.
Reference texts. K. Ogata, Modern Control Engineering, 5th ed. (Prentice Hall) — the source of this paper's problem style; N. S. Nise, Control Systems Engineering, 7th ed. (Wiley); R. C. Dorf and R. H. Bishop, Modern Control Systems, 13th ed. (Pearson); G. F. Franklin, J. D. Powell and A. Emami-Naeini, Feedback Control of Dynamic Systems, 8th ed. (Pearson).
Check: conventions used throughout. All transfer functions are written in the Laplace variable s with zero initial conditions unless a question states otherwise. “Unity feedback” means \(H(s)=1\), so the closed-loop transfer function is \(T(s)=G(s)/[1+G(s)]\) and the error signal is \(E(s)=R(s)-C(s)\). Root-locus gains are the gain \(K\) exactly as it appears in the printed \(G(s)\).
Question 2: Routh Stability — Range of Gain and an Open-Loop Unstable Plant (25 marks)
Given. Part (a): a type-1 loop with adjustable gain \(K\) and open-loop poles at \(s=0,\,-1,\,-2\). Part (b): a fixed-gain loop with poles at \(s=0,\,+1,\,-3/2\) — note the right-half-plane open-loop pole at \(s=+1\), which makes this an open-loop unstable plant.
Find. (a) all values of \(K\) for which the closed loop is stable, together with the frequency at which the roots cross the imaginary axis; (b) a definite yes/no verdict on the stability of the second loop, supported by the Routh array.
Approach. In both parts form the closed-loop characteristic polynomial \(1+G(s)=0\), clear denominators, and apply the Routh–Hurwitz criterion: the loop is stable if and only if every entry in the first column of the array is positive, and the number of sign changes equals the number of closed-loop poles in the right half plane.
Form the characteristic equation for part (a). With unity feedback the closed-loop poles satisfy \(1+G(s)=0\), i.e.
$$s(s+1)(s+2)+K=0\;\Longrightarrow\;s^3+3s^2+2s+K=0$$
All coefficients must be positive for stability, which already requires \(K>0\) — a necessary condition, but for a third-order polynomial not a sufficient one.
Build the Routh array. Writing the coefficients in the standard interleaved pattern:
$$\begin{array}{c|cc} s^3 & 1 & 2\\ s^2 & 3 & K\\ s^1 & \dfrac{3(2)-1(K)}{3}=\dfrac{6-K}{3} & 0\\ s^0 & K & \end{array}$$
Impose positivity of the first column. The entries are \(1,\;3,\;(6-K)/3,\;K\). The first two are positive automatically; the remaining two require
$$\frac{6-K}{3}>0\;\Rightarrow\;K<6,\qquad\text{and}\qquad K>0$$
so that
$$\boxed{\;0<K<6\;}$$
Locate the imaginary-axis crossing. At the upper limit \(K=6\) the \(s^1\) row vanishes, and the auxiliary polynomial is read from the row above it:
$$A(s)=3s^2+K=3s^2+6=0\;\Longrightarrow\;s^2=-2\;\Longrightarrow\;s=\pm j\sqrt{2}=\pm j1.4142$$
So at \(K=6\) the loop sustains an undamped oscillation at \(\omega=1.414\ \text{rad/s}\); the third root is at \(s=-3\). Substituting \(K=5.9\) and \(K=6.1\) into the cubic confirms numerically that the pair crosses from the left half plane into the right half plane as \(K\) passes 6.
Now part (b): form its characteristic equation. Expanding the open-loop denominator first,
$$s(s-1)(2s+3)=s\left(2s^2+s-3\right)=2s^3+s^2-3s$$
so \(1+G(s)=0\) gives
$$\boxed{\;2s^3+s^2-3s+10=0\;}$$
The coefficient of \(s\) is negative while the others are positive. Because a necessary condition for stability is that all coefficients of the characteristic polynomial share the same sign, the system can be declared unstable at this point — but the array tells us how unstable.
Complete the Routh array for part (b).
$$\begin{array}{c|cc} s^3 & 2 & -3\\ s^2 & 1 & 10\\ s^1 & \dfrac{1(-3)-2(10)}{1}=-23 & 0\\ s^0 & 10 & \end{array}$$
The first column is \(2,\;1,\;-23,\;10\): it changes sign twice (positive to negative, then negative to positive).
$$\boxed{\;\text{Two closed-loop poles lie in the right half plane}\;\Rightarrow\;\text{the system is UNSTABLE}\;}$$
Solving the cubic numerically confirms the count: the roots are approximately \(s=-1.7297\) and \(s=+0.6149\pm j1.6180\), i.e. one stable real root and an unstable oscillatory pair.
It is worth being explicit about why part (b) has no rescue. The gain is fixed at 10, so there is no free parameter to adjust; and even if the numerator gain were treated as variable, the negative \(s\)-coefficient of \(2s^3+s^2-3s+\text{(gain)}\) is contributed entirely by the plant, so no pure gain can remove it. Stabilising this plant requires dynamic compensation — a lead network or a state-feedback design that reshapes the coefficient itself.
Quantity
Result
(a) Characteristic equation
\(s^3+3s^2+2s+K=0\)
(a) Stability range
\(0<K<6\)
(a) Imaginary-axis crossing
\(s=\pm j\sqrt{2}=\pm j1.4142\) at \(K=6\)
(b) Characteristic equation
\(2s^3+s^2-3s+10=0\)
(b) Routh first column
\(2,\;1,\;-23,\;10\) — two sign changes
(b) Verdict
Unstable; 2 poles in the RHP (\(+0.615\pm j1.618\))