20-Bio-A2 Process Dynamics and Control · May 2018
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
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.
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.
| Result | Value |
|---|---|
| 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 | $K_{\max}=2.150$ |