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22-Mec-A3 System Analysis and Control · May 2014

Question 2 of 6: Routh–Hurwitz ranges of a parameter

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, May 2014 — 07-Mec-A3 System Analysis and Control. Closed book, 3 hours; a Casio or Sharp approved calculator and semi-log graph paper are the only aids. Six questions are printed; any four constitute a complete paper and all questions are of equal value (25 marks each). All six questions are solved in full. A Laplace-transform table is appended to the exam (pages 5–6) and two sheets of blank four-cycle semi-log paper are provided for the Bode work.

Reference texts. K. Ogata, Modern Control Engineering, 5th ed. (Pearson) — Chapters 5–7; N. S. Nise, Control Systems Engineering, 8th ed. (Wiley) — Chapters 6–10; 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). These are the standard Canadian undergraduate control texts and cover every technique used below (Routh–Hurwitz, root locus, Bode margins, static error constants, frequency response).

Notation. Throughout, K denotes the root-locus (pole–zero form) gain that multiplies the open-loop transfer function as printed, and ω is in rad/s. Magnitudes in decibels are 20 log10 of the magnitude ratio.

Question 2: Routh–Hurwitz ranges of a parameter (25 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Four third-order characteristic polynomials in which the single parameter $\alpha$ occupies a different coefficient position in each case:

CaseCharacteristic equationPosition of α
(a)$s^3+s^2+s+\alpha=0$constant term $a_0$
(b)$s^3+s^2+\alpha s+1=0$$s$ coefficient $a_1$
(c)$s^3+\alpha s^2+s+1=0$$s^2$ coefficient $a_2$
(d)$\alpha s^3+s^2+s+1=0$leading coefficient $a_3$

Find. For each case, the complete range of real $\alpha$ that places every root strictly in the open left half-plane (i.e. the range for which the system is asymptotically stable).

Approach. Build the Routh array once for the general cubic $a_3s^3+a_2s^2+a_1s+a_0$, extract the two independent conditions that its first column carries, then substitute each case in turn; a root-location check by direct factorisation confirms every boundary.

  1. Form the general Routh array. For $a_3s^{3}+a_2s^{2}+a_1s+a_0=0$ the array is $$\begin{array}{c|cc} s^{3} & a_3 & a_1\\ s^{2} & a_2 & a_0\\ s^{1} & \dfrac{a_2a_1-a_3a_0}{a_2} & 0\\ s^{0} & a_0 & \end{array}$$ All four first-column entries must share the same sign (conventionally all positive), which for a cubic collapses to the compact Hurwitz statement
  2. State the two stability conditions. Every coefficient must be positive and the middle-row test must hold: $$\boxed{\;a_3,a_2,a_1,a_0 > 0 \quad\text{and}\quad a_2a_1 > a_3a_0\;}$$ The first condition is necessary but not sufficient; the product condition is what actually detects the pair of complex roots crossing the imaginary axis.
  3. Case (a): $\alpha$ in the constant term. Here $a_3=a_2=a_1=1$ and $a_0=\alpha$. Positivity demands $\alpha > 0$; the product test gives $1\times 1 > 1\times\alpha$, i.e. $\alpha < 1$. Combining, $$\boxed{\;0 < \alpha < 1\;}$$ At $\alpha=1$ the polynomial factors as $(s+1)(s^{2}+1)$, confirming a pair of roots exactly on the imaginary axis at $s=\pm j1$; at $\alpha=0$ a root sits at the origin.
  4. Case (b): $\alpha$ multiplying $s$. Now $a_1=\alpha$ and $a_0=1$, so positivity requires $\alpha > 0$ and the product test requires $1\times\alpha > 1\times 1$. The second is the binding condition: $$\boxed{\;\alpha > 1\;}$$ There is no upper limit — increasing the $s$ coefficient adds damping without limit. At $\alpha = 1$ the polynomial is again $(s+1)(s^{2}+1)$.
  5. Case (c): $\alpha$ multiplying $s^{2}$. With $a_2=\alpha$, positivity gives $\alpha > 0$ and the product test gives $\alpha\times 1 > 1\times 1$, so once more $$\boxed{\;\alpha > 1\;}$$ Physically this is the same statement as case (b): the $s^{2}$ coefficient is the sum of the pole magnitudes, so it too must be large enough to keep the complex pair damped.
  6. Case (d): $\alpha$ as the leading coefficient. A negative $\alpha$ makes the coefficients change sign, so no root pattern can be stable; for $\alpha > 0$ the product test reads $1\times 1 > \alpha\times 1$. Hence $$\boxed{\;0 < \alpha < 1\;}$$ Note that $\alpha\to 0$ is a degenerate limit: the polynomial drops to second order ($s^{2}+s+1$, stable), but the third root has escaped to infinity, so the strict inequality is retained.
  7. Verify by root computation. Substituting representative values and factoring numerically confirms every range: $\alpha=0.5$ in (a) gives roots $-0.6478,\ -0.1761\pm j0.8607$ (all stable); $\alpha=1.5$ in (a) gives $-1.2041,\ 0.1020\pm j1.1115$ (unstable), and the same pattern of confirmation holds for (b), (c) and (d).

The four cases together make the pedagogical point of the question: the same cubic can be destabilised by making any one coefficient too small relative to the others, but which direction is "too small" depends on where the parameter sits. Parameters in $a_1$ or $a_2$ have lower bounds; parameters in $a_0$ or $a_3$ have upper bounds.

CaseCharacteristic equationStable range of α
(a)$s^3+s^2+s+\alpha=0$0 < α < 1
(b)$s^3+s^2+\alpha s+1=0$α > 1
(c)$s^3+\alpha s^2+s+1=0$α > 1
(d)$\alpha s^3+s^2+s+1=0$0 < α < 1