Anderson’s criterion and a combined gradient criterion are the two diagnostic checks you must apply. To keep intraparticle temperature-induced rate errors below 5%, ensure that the dimensionless product of the Thiele modulus, Prater number, and Arrhenius number is less than one. For positive‑order reactions where concentration and thermal gradients interact, a second, more restrictive condition involves the reaction order and must also be satisfied.
When using laboratory catalytic reactors, the non‑isothermal error in the observed rate stays below 5% if both Φ β γ < 1 (Anderson’s criterion) and, for positive‑order kinetics, Φ < 1/(n – β γ)—provided the denominator is not near zero. These simple calculations allow you to choose particle sizes and temperatures that maintain a virtually isothermal pellet.
The Dimensionless Numbers Behind the Criteria
The Thiele Modulus (Φ) – Reaction vs. Diffusion
The Thiele modulus, Φ, compares the intrinsic reaction rate to the rate of diffusion inside the catalyst pore. A small Φ means the pellet is fully utilized; a large Φ indicates severe internal concentration gradients. Φ depends on particle size, effective diffusivity, and the rate constant.
The Prater Number (β) – Maximum Possible Temperature Rise
The Prater number, β, represents the maximum relative temperature difference that could develop across the pellet. It is defined as the ratio of heat generation to heat conduction: β = (–ΔH) D_eff C_s / (λ_eff T_s). A small β means the pellet conducts heat so well that even under strong diffusion limitation, temperature gradients remain tiny.
The Arrhenius Number (γ) – Temperature Sensitivity
The Arrhenius number, γ = E/(RT_s), gauges how steeply the rate constant changes with temperature. A high γ makes the reaction exquisitely sensitive to even small temperature variations, amplifying the effect of the Prater‑driven gradient on the local rate.
Key Diagnostic Criteria
Anderson’s Criterion: The Isothermal “Safety Switch”
Anderson’s criterion combines all three numbers into a single product: Φ β γ < 1. When this inequality holds, the maximum temperature variation inside the pellet is small enough that the rate anywhere in the pellet deviates from the surface‑temperature rate by less than 5%. It is the quickest first check for any reaction system.
The Combined‑Gradient Criterion for Positive‑Order Reactions
Concentration and temperature gradients act together. For a reaction of order n, the interacting gradients can magnify the rate error even when Anderson’s criterion is marginally satisfied. To guard against that, a second check is required: Φ < 1/(n – β γ). This condition is more stringent when β γ is positive (exothermic reaction; heat release speeds up the reaction inside). Note that the denominator must not approach zero—that region corresponds to ignition/extinction phenomena and invalidates the simple 5%‑deviation analysis.
Applying the Criteria in the Laboratory
Step 1 – Gather Pellet and Reaction Data
You need the pellet radius (or characteristic length), effective diffusivity and thermal conductivity, surface concentration and temperature, heat of reaction, activation energy, and the intrinsic rate law (order n). Many of these can be estimated from correlations or measured separately.
Step 2 – Calculate Φ, β, and γ
Compute Φ from the observed rate and the effective diffusivity. Evaluate β and γ at the external‑surface conditions. Because the rate constant appears in Φ, an isothermal estimate can be used initially; iterative refinement is rarely needed if the criteria are comfortably met.
Step 3 – Check Both Inequalities
Start with Anderson’s criterion. If Φ β γ < 1, the pellet is practically isothermal for rate‑measurement purposes. For n‑th order kinetics, subsequently verify that Φ indeed lies below 1/(n – β γ). If either condition fails, intraparticle temperature gradients are causing more than 5% deviation from the isothermal rate.
Step 4 – Adjust if Criteria Fail
The most direct corrective action is to reduce the catalyst particle size. Φ scales with the pellet dimension, so crushing and sieving to a smaller fraction immediately shrinks both Φ and the product Φ β γ. Lowering the operating temperature also helps by decreasing γ and the rate constant (which reduces Φ), though it may slow data collection.
Understanding the Trade‑offs
Sensitivity to Parameter Uncertainty
Both criteria rely on accurate transport properties. Errors in effective diffusivity or thermal conductivity propagate directly into Φ and β. When using literature correlations, build a safety margin by targeting Φ β γ well below 0.5 rather than near 1.
The Ignition/Extinction Danger Zone
For strongly exothermic reactions, β γ can become large, pushing the denominator 1/(n – β γ) toward zero or negative. In that case the combined‑gradient criterion is meaningless: the pellet will exhibit multiple steady states, and 5%‑level analysis no longer applies. Operate far from this regime or switch to a differential reactor with a single, well‑mixed pellet bath.
Concentration Gradients May Still Exist
Satisfying the thermal criteria does not guarantee an absence of concentration gradients. You must separately check for pore‑diffusion limitations (e.g., using the Weisz‑Prater criterion) to ensure that the observed rate is truly the intrinsic kinetic rate. Temperature and concentration diagnostics are complementary.
Making the Right Choice for Your Goal
The criteria you apply depend on what kind of data you intend to collect and why.
- If your primary focus is measuring intrinsic kinetics: Shrink particles until Φ β γ ≪ 1 and Φ ≪ 1/(n – β γ). This ensures that both thermal and concentration gradients are negligible, giving you clean rate data.
- If your primary focus is screening catalysts under industrial pellet sizes: Compute Φ, β, and γ to know the magnitude of the expected deviation. Use the criteria to estimate the error and decide whether to correct the observed rate with an effectiveness‑factor model or to accept a known bias.
- If your primary focus is teaching reaction engineering concepts: Deliberately operate near the threshold to demonstrate the onset of non‑isothermal effects. The criteria become a predictive tool that students can validate by varying particle size and observing the rate change.
By making these dimensionless checks routine, you turn a potentially hidden error into a quantified, manageable variable—ensuring your laboratory data faithfully represents the true catalytic chemistry.
Summary Table:
| Diagnostic Criterion | Key Formula / Condition | Purpose & Application |
|---|---|---|
| Anderson's Criterion | Φ β γ < 1 | General check to ensure intraparticle rate deviation stays below 5%. |
| Combined-Gradient Criterion | Φ < 1/(n - β γ) | Accounts for interacting concentration and thermal gradients in positive-order kinetics. |
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