Introduction & Context
Reactive crystallization is a process where chemical reaction and crystallization occur simultaneously,
enabling precise control over particle size distribution (PSD), morphology, and polymorphism.
This calculation sheet focuses on the design of a reactive crystallization system for calcium carbonate (CaCO3),
a model system for studying precipitation kinetics, mixing effects, and particle engineering.
In Process Engineering, reactive crystallization is critical for:
- Producing high-purity, uniform particles (e.g., pharmaceuticals, pigments, catalysts).
- Controlling supersaturation to avoid fouling or agglomeration.
- Optimizing energy input (mixing) to balance nucleation and growth.
Typical applications include:
- Carbon capture (CO2 mineralization via CaCO3).
- Pharmaceutical active ingredient (API) synthesis.
- Specialty chemical manufacturing (e.g., nanoscale precipitates).
Methodology & Formulas
1. Temperature Conversion
Convert the process temperature from Celsius (\(T_C\)) to Kelvin (\(T_K\)):
\[
T_K = T_C + 273.15
\]
2. Reaction Kinetics (Arrhenius Law)
The temperature-dependent reaction rate constant (\(k\)) is calculated using the Arrhenius equation:
\[
k = k_{ref} \cdot \exp \left( -\frac{E_a}{R_g} \left( \frac{1}{T_K} - \frac{1}{T_{ref}} \right) \right)
\]
where:
- \(k_{ref}\): Rate constant at reference temperature \(T_{ref}\).
- \(E_a\): Activation energy (J/mol).
- \(R_g\): Universal gas constant (8.314 J/mol·K).
The reaction rate (\(r\)) for a bimolecular reaction (e.g., Ca(OH)2 + CO2 → CaCO3 + H2O)
is given by:
\[
r = k \cdot C_A^{\alpha} \cdot C_B^{\beta}
\]
where:
- \(C_A, C_B\): Concentrations of reactants A and B (mol/m³).
- \(\alpha, \beta\): Reaction orders for A and B.
3. Mixing Characterization
The Damköhler number (Da) quantifies the competition between reaction and mixing timescales:
\[
Da = r \cdot \tau_{mix}
\]
where \(\tau_{mix}\) is the mixing time (s), estimated from turbulent energy dissipation (\(\epsilon\)) and velocity fluctuations (\(u'\)):
\[
\tau_{mix} = \frac{\epsilon^{1/3}}{u'^2}
\]
The Reynolds number (Re) validates turbulent flow conditions:
\[
Re = \frac{\rho \cdot u' \cdot L}{\mu}
\]
where:
- \(\rho\): Fluid density (kg/m³).
- \(\mu\): Dynamic viscosity (Pa·s).
- \(L\): Characteristic length (m).
4. Supersaturation and Particle Size Control
Supersaturation (\(S\)) drives nucleation and growth. An empirical correlation links \(S\) to the target particle size (\(d_p\)):
\[
d_p \propto S^{-2}
\]
Rearranged to estimate the actual supersaturation (\(S_{actual}\)) for a given \(d_p\):
\[
S_{actual} = S_{target} \cdot \left( \frac{d_p}{d_{p,target}} \right)^{-1/2}
\]
5. Regime Criteria and Validity Checks
| Parameter |
Symbol |
Recommended Range |
Regime Implications |
| Damköhler Number |
\(Da\) |
\(10^{-6} < Da < 1\) |
- \(Da \gg 1\): Reaction-limited (mixing is fast).
- \(Da \ll 1\): Mixing-limited (reaction is fast).
|
| Supersaturation Ratio |
\(S\) |
\(1.1 < S < 2.0\) |
- \(S < 1.1\): Low nucleation; risk of slow growth.
- \(S > 2.0\): High nucleation; risk of fines/agglomeration.
|
| Turbulent Energy Dissipation |
\(\epsilon\) |
\(0.1 < \epsilon < 10\) W/kg |
- \(\epsilon < 0.1\): Poor mixing; inhomogeneous supersaturation.
- \(\epsilon > 10\): Excessive energy; potential particle breakage.
|
| Reynolds Number |
\(Re\) |
\(Re > 10,000\) |
- \(Re < 10,000\): Laminar flow; turbulent correlations invalid.
|
| Particle Size |
\(d_p\) |
\(1 < d_p < 100\) μm |
- \(d_p < 1\) μm: Colloidal range; filtration challenges.
- \(d_p > 100\) μm: Settling risk; suspension instability.
|
Worked Example – Sizing a Continuous Reactive Crystallizer for Precipitated Calcium Carbonate
A specialty-chemical plant must produce 150 kg h-1 of precipitated CaCO3 (mean crystal size 15 µm) by carbonating 0.1 mol L-1 Ca(OH)2 with 0.1 mol L-1 CO2 at 25 °C. The reaction is fast and mixing-controlled; we need to check whether the selected draft-tube crystallizer (L = 1 m, Re ≈ 105) can deliver the target supersaturation ratio S = 1.5 while keeping the Damköhler number below the micro-mixing limit.
Knowns
- Temperature: T = 25 °C (298.15 K)
- Rate constant at 25 °C: k25 = 0.005 s-1
- Activation energy: Ea = 30,000 J mol-1
- Reactant concentrations: CA0 = CB0 = 0.1 mol L-1
- Reaction orders: nA = nB = 1
- Target supersaturation: Starget = 1.5
- Target mean crystal size: dp = 15 µm
- Energy dissipation: ε = 1.0 m2 s-3
- Kinematic viscosity: ν = 1 × 10-6 m2 s-1
- Diffusivity: D = 1 × 10-9 m2 s-1
- Reactor length scale: L = 1.0 m
- Reynolds number: Re = 100,000
Step-by-step calculation
- Compute the intrinsic rate constant at 25 °C (already given):
k = 0.005 s-1
- Estimate the micro-mixing time (Bourne model) to compare with reaction time:
\[
\tau_{\text{mix}} = \left( \frac{L^2}{\epsilon} \right)^{1/3} = \left( \frac{1.0^2}{1.0} \right)^{1/3} = 1.0\ \text{s}
\]
- Calculate the Damköhler number for the bulk reaction:
\[
Da = \frac{k\ C_{\text{A0}}^{n_A-1}\ C_{\text{B0}}^{n_B-1}}{\tau_{\text{mix}}^{-1}} = \frac{0.005 \times 1}{1.0} = 0.005
\]
Since Da ≪ 1, mixing is faster than reaction and the system is kinetics-controlled.
- Determine the actual supersaturation generated at the chosen energy dissipation:
\[
S_{\text{actual}} = 1 + \frac{Da}{1 + Da} = 1 + \frac{0.005}{1 + 0.005} = 1.005 \approx 1.01
\]
To reach the target S = 1.5, raise the energy dissipation or reduce the mixing time. Re-arranging:
\[
\tau_{\text{mix,calc}} = \frac{k}{S_{\text{target}} - 1} = \frac{0.005}{0.5} = 0.01\ \text{s}
\]
The required specific power is therefore:
\[
\epsilon_{\text{req}} = \frac{L^2}{\tau_{\text{mix,calc}}^3} = \frac{1.0^2}{(0.01)^3} = 1 \times 10^6\ \text{m}^2\ \text{s}^{-3}
\]
- Check crystal size via the diffusion-limited growth expression:
\[
G = \frac{2\ D\ (S - 1)}{d_p} = \frac{2 \times 1 \times 10^{-9} \times 0.5}{15 \times 10^{-6}} = 6.7 \times 10^{-8}\ \text{m s}^{-1}
\]
For a mean residence time τ = 1800 s (30 min) the size increment is:
\[
\Delta L = G\ τ = 6.7 \times 10^{-8} \times 1800 = 0.00012\ \text{m} = 120\ \text{µm}
\]
Hence the target 15 µm is easily met within the chosen residence time.
Final Answer
Under the specified conditions, the crystallizer must operate at an energy dissipation of 1 × 106 m2 s-3 (≈ 1 kW kg-1) to achieve the target supersaturation ratio of 1.5, yielding a 15 µm mean CaCO3 crystal size with a 30-min residence time.