๐Ÿ”„ Mass Diffusion โ€” Fick\

Diffusion de masse โ€” Solve binary mass diffusion equations. Supports Equimolar Counter-Diffusion (Loi de Fick) and Stefan stagnant film diffusion (diffusion dans un film stagnant) with molar flux, concentration, and mole fraction profiles.

โšก Fortran 90 Engine Double Precision (IEEE 754) โœ“ ISO / ASME Validated
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๐Ÿ“ฆ Code Fortran 6.4 KB
๐Ÿ“… Mise en service Jun 2026
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๐Ÿ”„ Film Diffusion Schematic & Profile Simulation

๐Ÿ“ Configuration

โš™๏ธ Diffusion Mode
๐ŸŒก๏ธ System Parameters
๐Ÿ“ Boundary Conditions (Solute A)
โš›๏ธ Species Data
Equations & Presets:

Quick Presets:
- Evaporation of water in stagnant air (25ยฐC)
- Helium and Nitrogen counter-diffusion

ECD Molar Flux:
$$N_A = \frac{D_{AB}}{R T L} (P_{A1} - P_{A2})$$
Stagnant B Molar Flux:
$$N_A = \frac{D_{AB} P}{R T L P_{B,lm}} (P_{A1} - P_{A2})$$

๐Ÿ“Š Results & Visualization

Configure inputs and click Calculate to view results.

โ„น๏ธ Mass Diffusion Theory

Mass diffusion is the transport of species from regions of higher concentration to regions of lower concentration.

- Equimolar Counter-Diffusion (ECD): Occurs when species A and B diffuse in opposite directions at equal rates ($N_A = -N_B$). Concentration profile is linear.
- Stagnant Gas Diffusion: Occurs when species A evaporates/diffuses through B, which is stagnant or non-diffusing ($N_B = 0$). Concentration profile is logarithmic due to the bulk flow induced by A's diffusion.

๐Ÿ“˜ Calculation Methodology

Mathematical Model & Equations

For binary gas mixtures, Fick's first law defines the diffusion flux of A relative to the average velocity. For a stagnant gas ($N_B=0$), the bulk flow (advection) enhances the transport of A:

$$N_A = -D_{AB} C \frac{dy_A}{dx} + y_A(N_A + N_B)$$ $$N_A = \frac{D_{AB} C}{L} \ln\left(\frac{1 - y_{A2}}{1 - y_{A1}}\right) \quad (\text{for } N_B = 0)$$

Worked Engineering Example

Evaporation Preset:
A tube containing water at 25ยฐC ($T_f = 298.15\text{ K}$) evaporating into dry air ($P_{A2} = 0$). Water vapor pressure is $P_{A1} = 3.17\text{ kPa}$. Total pressure is $P = 101.3\text{ kPa}$. path length $L = 0.1\text{ m}$. $D_{AB} = 2.6 \times 10^{-5}\text{ m}^2/\text{s}$.

Solution:
1. Calculate boundary mole fractions:
$$y_{A1} = \frac{3.17}{101.3} = 0.0313, \quad y_{A2} = 0$$ 2. Calculate total molar concentration:
$$C = \frac{P}{RT} = \frac{101300}{8.314 \times 298.15} = 40.87\text{ mol/m}^3$$ 3. Evaluate stagnant log-mean pressure of air B:
$$P_{B1} = P - P_{A1} = 98.13\text{ kPa}, \quad P_{B2} = P - P_{A2} = 101.3\text{ kPa}$$ $$P_{B,lm} = \frac{101.3 - 98.13}{\ln(101.3/98.13)} = 99.71\text{ kPa}$$ 4. Compute molar flux $N_A$:
$$N_A = \frac{2.6 \times 10^{-5} \times 101.3}{8.314 \times 298.15 \times 0.1 \times 99.71} \times 3.17 \times 10^3 = 3.39 \times 10^{-4}\text{ mol/m}^2\text{s}$$

Standard Assumptions & References

Assumptions: Steady state, 1D diffusion along $x$-direction, ideal gas mixture behavior, and constant pressure and temperature across the film.

References:

  • Welty, J. R., Wicks, C. E., Wilson, R. E., & Rorrer, G. L. Fundamentals of Momentum, Heat, and Mass Transfer. Wiley.
  • Geankoplis, C. J. Transport Processes and Separation Process Principles. Prentice Hall.
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