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20-Bio-A5 Systems Analysis & Control · May 2017

Question 3 of 6: Batch Substrate-Inhibited Kinetics — Time to Half-Consume Substrate

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

Notes on this paper

National Exams / EGBC — May 2017 — 04-Bio-A5 Enzyme and Microbial Kinetics. Three-hour open-book examination; any non-communicating calculator is permitted. Six questions constitute a complete paper (10 + 25 + 15 + 20 + 15 + 15 = 100 marks). Content spans quasi-steady-state derivation of a substrate-inhibited enzyme mechanism, diffusion-reaction in an immobilized-enzyme bead (Thiele modulus / effectiveness factor), the rapid-equilibrium integrated batch equation for substrate inhibition, a growth-associated-product batch fermentation, Contois-kinetics chemostat design, and fed-batch quasi-steady-state theory.

Reference texts: Bailey & Ollis, Biochemical Engineering Fundamentals (2nd ed.) — enzyme kinetics, substrate inhibition, immobilized-enzyme diffusion-reaction and effectiveness factors, Monod/Contois growth models, chemostat and fed-batch theory. All quantities are used exactly as printed on the exam (SI/CGS mixed units as given).

Question 3: Batch Substrate-Inhibited Kinetics — Time to Half-Consume Substrate (15 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. Rapid-equilibrium substrate-inhibition rate law $v=\dfrac{V_{\max}S}{K_m'+S+S^2/K_s}$; $S_0=10$ mol/L, $K_m'=5$ mol/L, $K_s=1$ mol/L; $V_{\max}$ (i.e. $k_2E_0$) is not given numerically.

Find. The time $t_{1/2}$ for $S$ to fall to $S_0/2$, expressed in terms of the unknown $V_{\max}$; and the behaviour of this result as $S_0\to0$ compared with the non-inhibited (simple Michaelis–Menten) batch case.

Approach. Write the batch mass balance $-dS/dt=v$, separate variables, and integrate the rapid-equilibrium rate law in closed form — the reactor volume $V_L$ cancels (it appears on both sides of a concentration-based balance) so it never enters the answer.

  1. Batch balance. $$-\frac{dS}{dt}=\frac{V_{\max}S}{K_m'+S+S^2/K_s}.$$
  2. Separate and integrate. $$-\left(\frac{K_m'}{S}+1+\frac{S}{K_s}\right)dS=V_{\max}\,dt \ \Rightarrow\ K_m'\ln\frac{S_0}{S}+(S_0-S)+\frac{S_0^2-S^2}{2K_s}=V_{\max}t.$$
  3. Evaluate at $S=S_0/2=5$ mol/L. $$5\ln 2+(10-5)+\frac{10^2-5^2}{2(1)}=3.466+5.000+37.500=45.97,$$ so $$\boxed{t_{1/2}=\frac{45.97}{V_{\max}}}$$ (time units follow from those of $V_{\max}$, e.g. minutes if $V_{\max}$ is in mol/(L·min)).
  4. Limit $S_0\to0$. As $S_0\to0$ (with $S=S_0/2\to0$ too), the quadratic term $(S_0^2-S^2)/(2K_s)$ vanishes as $S_0^2$, strictly faster than the logarithmic and linear terms, so the integrated equation collapses to $$K_m'\ln\frac{S_0}{S}+(S_0-S)=V_{\max}t,$$ which is exactly the classical integrated batch equation for a non-substrate-inhibited (simple Michaelis–Menten) reaction with Michaelis constant $K_m'$. In other words, substrate inhibition is a high-concentration effect; at vanishingly small $S_0$ the inhibition term contributes nothing and $t_{1/2}$ approaches the plain-MM value using the same $K_m'$.
ResultValue
$t_{1/2}\cdot V_{\max}$ coefficient45.97 (mol/L)
$t_{1/2}$$45.97/V_{\max}$
$S_0\to0$ limiting equation$K_m'\ln(S_0/S)+(S_0-S)=V_{\max}t$ (plain MM)