POLLUTEv10 Example 9: Diffusion with Freundlich Non-Linear Sorption (Phenol in Clay)

POLLUTEv10 simulation of phenol diffusion in clay with Freundlich non-linear sorption and finite mass source
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In POLLUTEv10 Example 9, the model advances beyond linear sorption by incorporating Freundlich non-linear sorption to simulate the diffusion of phenol through a clay specimen. This example reflects more realistic contaminant behavior, particularly for organic compounds that do not follow simple linear partitioning.


Problem Overview

This example simulates a laboratory diffusion test with the following conditions:

  • Contaminant: Phenol
  • Soil: Clay (7 cm thick)
  • Transport mechanism: Diffusion only (no advection)
  • Sorption model: Freundlich non-linear isotherm
  • Bottom boundary: Impermeable (zero flux)
  • Source type: Finite mass

Source Conditions

  • Initial concentration (co): 50 mg/L
  • Leachate head (Hr): 6.5 cm

Times of Interest

  • 200 hr
  • 400 hr
  • 600 hr
  • 800 hr

Conceptual Model

The system consists of:

  • A finite mass source of phenol at the top
  • A clay layer where diffusion and sorption occur
  • An impermeable base preventing downward flux

Unlike constant concentration sources, the finite source means:

  • Concentration at the top decreases over time
  • Transport is influenced by both diffusion and depletion

Input Parameters

PropertySymbolValueUnits
Darcy Velocityva0.0cm/hr
Diffusion CoefficientD0.019cm²/hr
Freundlich CoefficientKf2.0cm³/g
Sorption Exponent0.628
Soil Porosityn0.46
Dry Density1.47g/cm³
Soil Layer ThicknessH7.0cm
Number of Sub-layers14
Source Concentrationco50.0mg/L
Leachate HeightHr6.5cm

Understanding Freundlich Non-Linear Sorption

The Freundlich isotherm describes sorption as:

S=KfCnS = K_f \, C^n

Where:

  • S = sorbed concentration
  • C = լուծ dissolved concentration
  • Kf = sorption capacity
  • n = non-linearity exponent

Key Implications

  • Sorption is not constant (unlike linear Kd models)
  • Retardation varies with concentration
  • Transport becomes concentration-dependent

With n = 0.628 (< 1):

  • Sorption is stronger at lower concentrations
  • This causes tailing effects in concentration profiles

Key Processes Simulated

1. Diffusion

  • Governed by concentration gradients
  • Slower compared to Example 8 due to lower diffusion coefficient

2. Non-Linear Sorption

  • Phenol interacts with clay via Freundlich behavior
  • Retardation is dynamic, not constant

3. Finite Mass Source

  • Source concentration decreases over time
  • Results in attenuated diffusion fronts

4. Boundary Condition

  • Zero flux at base → contaminant accumulates within the domain

Importance of Layer Discretization

This example highlights a critical modeling requirement:

Accuracy depends strongly on the number of sub-layers when using non-linear sorption.

Why?

  • Non-linear equations require finer resolution
  • Concentration-dependent retardation must be captured precisely
  • Coarse discretization can lead to numerical errors

Best Practice

  • Use ≥ 14 sub-layers (as in this example)
  • Increase layers further for higher accuracy or steeper gradients

Graphical Output: Depth vs Concentration


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Concentration Profiles

  • Profiles evolve over time (200 → 800 hr)
  • Slower migration compared to conservative solutes
  • Gradual flattening due to source depletion

Non-Linear Effects

  • Stronger sorption at low concentrations causes extended tails
  • Profiles are non-symmetric and more complex

Finite Source Behavior

  • Peak concentrations decrease over time
  • Diffusion front weakens as source mass is exhausted

Practical Applications

This example is especially relevant for:

  • Organic contaminant transport (e.g., phenol, hydrocarbons)
  • Landfill leachate assessments
  • Clay liner performance evaluation
  • Risk assessment modeling

It is particularly important when:

  • Contaminants exhibit non-linear adsorption
  • Long-term predictions are required
  • Laboratory calibration data is available

Best Practices for POLLUTEv10 Users

  • Always verify Freundlich parameters (Kf and n) from lab data
  • Use fine discretization for non-linear problems
  • Compare results at multiple time steps
  • Be cautious when interpreting retardation (not constant!)

Conclusion

POLLUTEv10 Example 9 demonstrates how incorporating Freundlich non-linear sorption significantly enhances the realism of contaminant transport modeling.

Key takeaways:

  • Non-linear sorption leads to concentration-dependent transport
  • Finite sources introduce time-varying boundary conditions
  • Numerical accuracy depends heavily on layer discretization

This example is essential for modeling organic contaminants in clay systems, where linear assumptions are often insufficient.


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