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23-Chem-B4 Biochemical Engineering · May 2014

Question 2 of 6: Internal Diffusion Limitation in Immobilized Enzyme Beads

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

Notes on this paper

National Exam 04-Chem-B4, Biochemical Engineering — May 2014. 3 hours, Closed-Book Exam (any non-communicating calculator permitted). Six questions are printed; per the exam notes any five (5) constitute a complete paper (100 marks) and only the first five as they appear in the answer book are marked. All six are solved below for completeness.

Reference texts: Shuler & Kargi, Bioprocess Engineering: Basic Concepts, 2nd ed.; Bailey & Ollis, Biochemical Engineering Fundamentals, 2nd ed.; Madigan et al., Brock Biology of Microorganisms, 13th ed.

Question 2: Internal Diffusion Limitation in Immobilized Enzyme Beads (20 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.

QuantitySymbolValue
First-order rate constantk13.6 h-1 = 1.0×10-3 s-1
Bead radiusR6 mm = 6×10-3 m
Effective substrate diffusivityDe1×10-6 m²/s
Strip volumeVp1×10-9 m³
Strip surface areaSp6×10-6 m²

Find. (i) Whether internal (intraparticle) diffusion limits the observed reaction rate in the spherical bead; (ii) how the same test changes when the particle shape is a thin rectangular strip.

Approach. Use the generalized (Aris-normalized) Thiele modulus $\phi=(V_p/S_p)\sqrt{k_1/D_e}$, built from each particle's own volume-to-surface ratio as its characteristic diffusion length. This normalization makes the same numeric criterion — φ ≪ 1 ⇒ reaction-limited (η ≈ 1, substrate not limiting); φ ≫ 1 ⇒ diffusion-limited (η ≈ 1/φ) — apply to any particle shape, sphere or strip alike.

C(r) ≈ Cₛ throughout(φₛ ≈ 0.063 ≪ 1, reaction-limited)R = 6 mmspherical beadVₚ/Sₚ = R/3 = 2.0 mmthin striprectangular stripVₚ/Sₚ = 0.167 mm (12× thinner)φₛₜᵣᵢₚ ≈ 0.0053 (even flatter profile)Fig. 2 — characteristic diffusion length Vₚ/Sₚ sets the Thiele modulus (both geometries are reaction-limited; the strip more so)
Fig. 2 — characteristic diffusion length Vp/Sp for the sphere vs. the strip.
  1. Common rate/diffusion ratio. Both geometries share the same intrinsic kinetics and diffusivity, so compute $\sqrt{k_1/D_e}$ once: $$\sqrt{\frac{k_1}{D_e}}=\sqrt{\frac{1.0\times10^{-3}\ \text{s}^{-1}}{1\times10^{-6}\ \text{m}^2/\text{s}}} =\sqrt{1000\ \text{m}^{-2}}=\boxed{31.6\ \text{m}^{-1}}$$
  2. (i) Thiele modulus for the sphere. A sphere's volume-to-surface ratio is $V_p/S_p=(\tfrac{4}{3}\pi R^3)/(4\pi R^2)=R/3$: $$\frac{V_p}{S_p}\Big|_{sphere}=\frac{6\times10^{-3}}{3}=2.0\times10^{-3}\ \text{m}$$ $$\phi_{sphere}=(2.0\times10^{-3})(31.6)=\boxed{0.0632}$$ Since $\phi_{sphere}=0.063\ll1$ (well below the ≈0.3 threshold for the onset of diffusion control), the effectiveness factor $\eta\approx1$: the reaction, not substrate diffusion, is rate-limiting — substrate availability is NOT a limiting factor for the 6 mm bead.
  3. (ii) Thiele modulus for the strip. The strip's own $V_p/S_p$ replaces R/3 as the characteristic length: $$\frac{V_p}{S_p}\Big|_{strip}=\frac{1\times10^{-9}\ \text{m}^3}{6\times10^{-6}\ \text{m}^2} =1.67\times10^{-4}\ \text{m}$$ $$\phi_{strip}=(1.67\times10^{-4})(31.6)=\boxed{5.27\times10^{-3}}$$ $\phi_{strip}/\phi_{sphere}=0.083$: the strip's characteristic diffusion path is about 12× shorter than the bead's, so its Thiele modulus is proportionally smaller. It is still (even more clearly) reaction-limited — substrate availability remains not limiting, and the strip geometry moves the system further into the reaction-limited regime, not closer to diffusion control.
QuantityValueRegime
√(k1/De)31.6 m-1—
φsphere (bead, R=6 mm)0.0632reaction-limited, η≈1
φstrip0.00527reaction-limited, η≈1 (more so)