Reference ID: MET-EADA | Process Engineering Reference Sheets Calculation Guide
Introduction & Context
The Noyes–Whitney equation is the classical mass-transfer model for dissolution of a solid into a well-stirred liquid. In pharmaceutical and chemical process engineering, it is used to predict the instantaneous in-vitro dissolution rate of tablets, granules, or powders under controlled hydrodynamic conditions (USP paddle/basket apparatus, flow-through cells, etc.). Accurate rate estimates are required for:
Formulation screening and excipient selection
Scaling from lab to production (equipment similarity)
Justifying biowaiver requests via in-vitro–in-vivo correlations (IVIVC)
Detecting possible mass-transfer limitations in crystallisation or reactive systems
Methodology & Formulas
The model treats the solid–liquid interface as a planar surface bathed by a stagnant diffusion film of thickness h. Solute molecules migrate across this film under the influence of the concentration gradient. The process is assumed to be:
Isothermal and isobaric
Sink or near-sink (bulk concentration Cb ≪ Cs)
Film-controlled (surface reaction much faster than diffusion)
Step 1 – Convert film thickness to centimetres
\[ h_{\text{cm}} = h_{\mu m} \times 10^{-4} \]
Step 2 – Impose a minimum gradient to avoid division by zero
Recommended hydrodynamic regime for standard USP II apparatus
Parameter
Range
Interpretation
Film thickness h
30–100 µm
Corresponds to 50–150 rpm paddle speed
Sink index
Cb ≤ 0.3 Cs
Ensures gradient remains essentially Cs
Outside these intervals, the assumptions of a single stagnant film and/or constant gradient may no longer hold; experimental calibration or more elaborate mass-transfer correlations (e.g., Levich, Ranz–Marshall) should be used instead.
The Noyes-Whitney equation, \(\frac{dm}{dt} = k A (C_s - C_t)\), states that the dissolution rate is proportional to the surface area of the solid and the concentration gradient. For process engineers, it is the quantitative link between particle size, agitation, solubility, and time; use it to predict how long your active will stay in the vessel before reaching target concentration and to avoid over-milling or under-mixing.
Reduce particle size via in-line high-shear rotor–stator or recirculation through a wet mill to increase A.
Raise impeller tip speed (within power-draw limits) to cut boundary-layer thickness and raise the mass-transfer coefficient k.
Increase temperature to boost Cs while watching for thermal degradation or solvent losses.
Adjust pH or add permitted co-solvent if Cs is pH-dependent; verify compatibility with downstream ion-exchange or crystallization.
Use dimensional analysis: calculate Sherwood (Sh = k L/D), Reynolds (Re = ρ N D2/μ), and Schmidt (Sc = μ/ρ D) numbers from pilot data. Maintain constant Sh at equal Sc to scale k; compensate for lower specific power (W kg-1) in the larger tank by increasing impeller diameter or adding a second impeller while keeping tip speed below shear-sensitive limits. Validate with a 200–500 L demonstration batch before GMP campaign.
Check three common failures:
Surface area shrinkage—particles agglomerate or float; verify adequate suspension by measuring just-suspended speed (Njs) with Zwietering correlation.
Concentration at saturation—Ct ≈ Cs; sample and confirm Cs at process temperature; if undissolved solid persists, solubility may have been over-estimated.
Mass-transfer limitation—k drops when viscosity rises from dissolved excipients; introduce baffles or switch to pitched-blade turbine to improve top-to-bottom turnover.
Worked Example – Estimating Dissolution Rate for a New Immediate-Release Tablet
A process engineer is scaling-up a wet-granulation line for an immediate-release tablet whose active pharmaceutical ingredient (API) is sparingly soluble. To size the granulation vessel and set the in-line dissolution target, the engineer needs the theoretical dissolution rate predicted by the Noyes–Whitney equation.
Knowns
Effective surface area exposed to the medium, A = 1.3 cm²
Diffusion coefficient of the API in water at 37 °C, D = 0.0012 cm² s⁻¹
Static boundary-layer thickness, h = 50 µm = 0.005 cm
Solubility limit in the diffusion layer, Cs = 1.5 mg cm⁻³
Determine the intrinsic mass-transfer coefficient for the stagnant film:
\[
k = \frac{D}{h} = \frac{0.0012}{0.005} = 0.240\ \text{cm s}^{-1}
\]
Combine area and coefficient to obtain the volumetric mass-transfer term:
\[
kA = 0.240 \times 1.3 = 0.312\ \text{cm}^{3}\ \text{s}^{-1}
\]
Apply the Noyes–Whitney rate expression:
\[
\frac{dm}{dt} = kA\,\nabla C = 0.312 \times 1.5 = 0.468\ \text{mg s}^{-1}
\]
Convert to more convenient process units:
\[
0.468\ \text{mg s}^{-1} \times 60\ \text{s min}^{-1} = 28.1\ \text{mg min}^{-1}
\]
Final Answer
The API is predicted to dissolve at 0.468 mg s⁻¹ (≈ 28.1 mg min⁻¹) under the specified hydrodynamic and sink conditions. This value sets the upper bound for the granulation vessel’s mass-transfer requirement and can be compared with subsequent in-line UV dissolution data to verify process performance.
"Un projet n'est jamais trop grand s'il est bien conçu."— André Citroën
"La difficulté attire l'homme de caractère, car c'est en l'étreignant qu'il se réalise."— Charles de Gaulle