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20-Bio-A2 Process Dynamics and Control · May 2018

Question 3 of 8: Phase Margin, Gain Margin and Maximum Stable Gain for a Dead-Time Process

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

Notes on this paper

National Exams / EGBC — May 2018 — 04-Bio-A2 Process Dynamics and Control. Three-hour open-book examination; any non-communicating calculator is permitted. The cover page states that only the first five questions in the answer book are marked, yet all eight problems are printed on the paper — all eight are solved below for completeness, since the full set is a study resource. Content spans second-order Bode/phase-margin analysis, feedback stability with a non-minimum-phase sensor, dead-time Nyquist/gain-margin design, zero-location effects on step response, nonlinear radiative-heat-transfer linearization, Internal Model Control (IMC) of a dead-time process, PI-controller stability/response, and nonlinear-CSTR linearization. Note: Problem 2's printed sub-part weights (10%+20%=30%) exceed its stated 20% problem total — both sub-parts are fully answered below.

Reference texts: D. E. Seborg, T. F. Edgar, D. A. Mellichamp & F. J. Doyle III, Process Dynamics and Control (4th ed., Wiley) — Laplace-domain modelling, transfer functions, Routh stability, Nyquist/Bode frequency response, linearization and IMC design; G. Stephanopoulos, Chemical Process Control: An Introduction to Theory and Practice (Prentice Hall) — Nyquist criterion and dead-time systems. Standard control conventions (deviation variables; unity valve gain unless stated) are used throughout.

Problem 3: Phase Margin, Gain Margin and Maximum Stable Gain for a Dead-Time Process (20%)

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. Open-loop $L(s)=K\dfrac{e^{-0.5s}}{s(s+1)}$, dead time $\theta=0.5\ \text{s}$, integrator plus first-order lag.

Find. (1) PM and GM at $K=1$; (2) the exact maximum $K$ for closed-loop stability.

Approach. Write the exact magnitude and phase of $L(j\omega)$ (the dead time contributes phase only, never magnitude); solve the gain-crossover condition $|L|=1$ in closed form; solve the transcendental phase-crossover condition numerically to full precision; then GM $=1/|L(j\omega_{pc})|$ and, since $K$ only scales magnitude, $K_{\max}=$ GM.

  1. Frequency response. $$|L(j\omega)|=\frac{K}{\omega\sqrt{\omega^2+1}},\qquad \angle L(j\omega)=-0.5\omega\,(\text{rad})-90^{\circ}-\arctan\omega.$$
  2. (1) Gain crossover at $K=1$. $|L(j\omega_{gc})|=1\Rightarrow\omega^2(\omega^2+1)=1$. With $x=\omega^2$: $x^2+x-1=0\Rightarrow x=\tfrac{\sqrt5-1}{2}$, so $$\boxed{\omega_{gc}=\sqrt{\tfrac{\sqrt5-1}{2}}=0.786\ \text{rad/s}.}$$
  3. (1) Phase margin. At $\omega_{gc}=0.786$: $-0.5(0.786)\cdot\tfrac{180}{\pi}=-22.52^{\circ}$, $-\arctan(0.786)=-38.16^{\circ}$; total phase $=-22.52-90-38.16=-150.68^{\circ}$, so $$\boxed{\text{PM}=180^{\circ}-150.68^{\circ}=29.31^{\circ}.}$$
  4. Phase crossover (exact, solved numerically). Setting $\angle L=-180^{\circ}$ gives the transcendental equation $0.5\omega+\arctan\omega=\pi/2$. Newton–Raphson converges to full precision: $$\boxed{\omega_{pc}=1.3065\ \text{rad/s}.}$$
  5. (1) Gain margin at $K=1$. $|L(j\omega_{pc})|=\dfrac{1}{1.3065\sqrt{1.3065^2+1}}=0.4652$, so $$\boxed{\text{GM}=\frac{1}{0.4652}=2.150\ (6.65\ \text{dB}).}$$
  6. (2) Maximum stable gain. The controller gain $K$ scales $|L|$ uniformly without changing its phase, so the phase-crossover frequency is unchanged for any $K$; instability begins exactly when $K|L_1(j\omega_{pc})|=1$, i.e. $$\boxed{K_{\max}=\text{GM}=2.150.}$$
ResultValue
Gain-crossover frequency ($K=1$)$\omega_{gc}=0.786\ \text{rad/s}$
Phase margin ($K=1$)$\text{PM}=29.31^{\circ}$
Phase-crossover frequency$\omega_{pc}=1.3065\ \text{rad/s}$
Gain margin ($K=1$)$\text{GM}=2.150\ (6.65\ \text{dB})$
Maximum stable gain$K_{\max}=2.150$