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23-Chem-A6 Process Dynamics and Control · December 2018

Question 7 of 8: Bode Plot and Gain Margin of a First-Order-Plus-Dead-Time Process

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

Notes on this paper

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, linearisation, transfer functions, feedback stability, frequency response and IMC design; G. Stephanopoulos, Chemical Process Control: An Introduction to Theory and Practice (Prentice Hall) — Routh test, Nyquist criterion, dead-time systems and state-space models; D. R. Coughanowr & S. E. LeBlanc, Process Systems Analysis and Control (3rd ed., McGraw-Hill) — first-order tank/thermal dynamics, step/impulse response and block-diagram algebra. Standard control conventions (deviation variables; unity valve/sensor gains unless stated) are used throughout. This sitting is an open-book paper of eight problems of which any five constitute a complete exam; all eight are solved here.

Problem 7: Bode Plot and Gain Margin of a First-Order-Plus-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. A FOPDT process under proportional control:

QuantityValue
Static gain$1$ ($0$ dB)
Time constant$\tau=0.5$ s $\Rightarrow \omega_c=2$ rad/s
Dead time$\theta=0.1$ s
Target gain margin$\mathrm{GM}=1.7$

Find. (a) the asymptotic Bode magnitude and phase; (b) $K_c$ giving $\mathrm{GM}=1.7$.

Asymptotic Bode plot (log $\omega$) $|G|$ (dB) slope 0 (0 dB) $-20$ dB/dec $\omega_c=2$ 0 phase (deg) $-90°$ $-180°$ 0 $\omega_{pc}\approx16.9$ lag: $-\arctan(0.5\omega)-0.1\omega$ delay drives phase past $-180°$
Problem 7: the magnitude is flat at $0$ dB to the corner $\omega_c=2$ rad/s, then falls at $-20$ dB/dec. The phase is the first-order lag plus the linearly-growing delay term $-0.1\omega$ (rad), so it crosses $-180^\circ$ at a finite $\omega_{pc}\approx16.9$ rad/s — only the dead time makes a phase crossover possible.

Approach. Build the Bode asymptotes from the first-order lag and the delay, find the phase-crossover frequency $\omega_{pc}$ where $\angle G=-180^\circ$, evaluate $|G(\omega_{pc})|$, and set $K_c$ so that $\mathrm{GM}=1/(K_c|G(\omega_{pc})|)=1.7$.

  1. (a) Magnitude asymptotes. The delay has unit magnitude, so $|G|=1/\sqrt{1+(0.5\omega)^2}$: flat at $0$ dB for $\omega\ll2$, breaking at the corner $\omega_c=1/\tau=2$ rad/s, then rolling off at $-20$ dB/decade. As $\omega\to\infty$, $|G|\to0$.
  2. (a) Phase. $\angle G=-\arctan(0.5\omega)-0.1\omega$ (rad). The lag contributes $0^\circ\to-90^\circ$ (passing $-45^\circ$ at $\omega_c=2$); the delay adds $-0.1\omega$ rad $=-5.73\omega$ degrees, unbounded. Hence the phase decreases without limit — the delay is what allows a $-180^\circ$ crossover.
  3. Phase crossover. Set $\angle G=-\pi$: $\arctan(0.5\omega)+0.1\omega=\pi$. Solving numerically gives $$\omega_{pc}=16.89\ \text{rad/s}.$$
  4. Magnitude at crossover. $|G(\omega_{pc})|=\dfrac{1}{\sqrt{1+(0.5\cdot16.89)^2}}=\dfrac{1}{\sqrt{1+71.3}}=0.1176.$
  5. (b) Gain for GM $=1.7$. With proportional control $L=K_cG$, the gain margin is $\mathrm{GM}=\dfrac{1}{K_c|G(\omega_{pc})|}$. Setting it to $1.7$: $$\boxed{K_c=\frac{1}{1.7\,|G(\omega_{pc})|}=\frac{1}{1.7(0.1176)}=5.0.}$$ At this gain the open-loop magnitude at the $-180^\circ$ frequency is $1/1.7\approx0.59$, i.e. $1.7\times$ below the stability limit.
QuantityValue
Corner frequency$\omega_c=2$ rad/s ($-20$ dB/dec above)
Phase-crossover freq.$\omega_{pc}=16.89$ rad/s
$|G(\omega_{pc})|$$0.1176$
(b) $K_c$ for GM $=1.7$$K_c=5.0$