23-Chem-B4 Biochemical Engineering · Undated paper
Question 3 of 5: Effective Diffusivity in an Immobilized-Enzyme Bead from the Observed Thiele Modulus
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exam 16-Chem-B4, Biochemical Engineering — May 2019 (the header on page 1 reads "16-Chem-B4/May 2019"). 3 hours, Closed-Book Exam (approved Casio or Sharp calculator
permitted). Per the exam notes, FIVE (5) questions constitute a complete paper and all five must be answered;
each question is of equal value (20 marks) and short-essay-format answers are marked for clarity and
organization.
Interpretation notes: Two points where the printed question itself needs an interpretation are flagged where they are used: the meaning of p in the Question 1 solubility equation, and the definition of the observable Thiele modulus in Question 3.
Question 3: Effective Diffusivity in an Immobilized-Enzyme Bead from the Observed Thiele Modulus (20 marks)
Convention note (exam Note 1): the observable Thiele modulus is defined here as in Shuler &
Kargi, with the characteristic length Vp/Sp = R/3 for a sphere:
Φ = (R/3)²robs/(DeS0). This matches the Thiele modulus
φ = (R/3)√(k/De) used in that text. The Weisz–Prater form in Fogler and in Bailey & Ollis uses R²
instead; with the same data it gives De = 1.94×10−9 m²/s, exactly 9 times
larger. That value is about three times the diffusivity of glucose in free water, which is not physically
reasonable for diffusion inside a particle, so the R/3 convention is preferred. S0 is taken as the
substrate concentration at the particle surface (no external film resistance).
Given.
Quantity
Symbol
Value
Particle diameter
dp
1 mm
Particle radius
R
0.5 mm = 5×10−4 m
Observed reaction rate
robs
200 μmol/(cm³ catalyst·min)
Initial (surface) substrate concentration
S0
100 mol/m³
Observable Thiele modulus
Φ
4.3
Find. The effective diffusivity De of the substrate inside the bead (m²/s).
Fig. 2 — immobilized-enzyme bead: strong internal diffusion limitation (Φ=4.3) leaves
the particle core substrate-starved (schematic, qualitative profile only — polyline truncated by the
plotting window for the steepest part of the curve).
Approach. Convert the observed rate to SI units, then use the observable Thiele modulus. It
is built only from quantities measured on the working particle (size, observed rate, surface concentration)
plus De, so no intrinsic rate constant is needed and it can be solved directly for De.
Observed rate in SI units. 1 μmol = 10−6 mol, 1 cm³ =
10−6 m³ and 1 min = 60 s, so
$$r_{obs}=\frac{200\times10^{-6}\ \text{mol}}{(10^{-6}\ \text{m}^3)(60\ \text{s})}=\boxed{3.333\ \text{mol}/(\text{m}^3\cdot\text{s})}$$
Observable modulus definition. For a sphere the characteristic length is
$V_p/S_p=R/3$, and
$$\Phi=\eta\,\phi^2=\left(\frac{R}{3}\right)^2\frac{r_{obs}}{D_e\,S_0},\qquad\frac{R}{3}=\frac{5\times10^{-4}}{3}=1.667\times10^{-4}\ \text{m}$$
Unlike the intrinsic modulus $\phi=(R/3)\sqrt{k/D_e}$, this group needs no intrinsic rate constant.
Rearrange and substitute.
$$D_e=\frac{(R/3)^2\,r_{obs}}{\Phi\,S_0}=\frac{(1.667\times10^{-4})^2\times3.333}{4.3\times100}=\frac{9.259\times10^{-8}}{430}$$
$$\boxed{D_e=2.15\times10^{-10}\ \text{m}^2/\text{s}}$$
Interpretation. Φ = 4.3 is well above 1, so pore diffusion strongly limits the rate: the
substrate is consumed before it can reach the particle centre, leaving a starved core (Fig. 2). The value of
De is about one-third of the diffusivity of a small sugar such as glucose in free water (about
6.7×10−10 m²/s), which is typical for diffusion through a gel or porous support.