POLLUTEv10 Example 7: Lateral Migration of a Radioactive Contaminant in Fractured Rock

POLLUTEv10 Example 7 diagram showing radioactive contaminant transport through fractured rock with advective-dispersive flow, matrix diffusion, and radioactive decay
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This example demonstrates how POLLUTEv10 can be used to simulate the lateral migration of a radioactive contaminant in a fractured porous rock system. It focuses on transport along a single set of parallel fractures, incorporating advection, dispersion, matrix diffusion, and radioactive decay.

The scenario is particularly relevant for nuclear waste disposal assessments, deep geological repositories, and long-term contaminant fate modeling.


Conceptual Model Overview

The model assumes:

  • A fractured rock domain extending effectively infinitely from the source
  • Transport occurring primarily along fractures (fast pathways)
  • Diffusion into the surrounding rock matrix (slow storage zone)
  • A radioactive contaminant that undergoes decay over time

The analysis focuses on:

  • First 50 m of transport distance
  • Time period of 30 years

Key Modeling Assumptions

  • Initial source concentration: co = 1 (normalized unit)
  • The source is constant (no depletion) due to large supply
  • Radioactive decay occurs continuously
  • No sorption in fractures or matrix (Kf = Km = 0)
  • Transport is governed by:
    • Advection
    • Dispersion
    • Matrix diffusion
    • First-order radioactive decay

Governing Radioactive Decay

The decay of the contaminant follows first-order kinetics:

C(t)=C0eλtC(t)=C_0 e^{-\lambda t}

Where:

  • C(t)C(t)= concentration at time ttt
  • C0C_0 = initial concentration
  • λ\lambda = decay constant
  • tt = time (years)

The decay constant is related to half-life:

λ=ln(2)t1/2=0.6931000.00693a1\lambda = \frac{\ln(2)}{t_{1/2}} = \frac{0.693}{100} \approx 0.00693 \, \text{a}^{-1}

This means that over 30 years, only modest decay occurs, making transport processes dominant in plume evolution.


Input Parameters

Hydraulic and Transport Properties

PropertySymbolValueUnits
Darcy Velocityva0.08m/a
Dispersion in fracturesDf6m²/a
Matrix diffusion coefficientDm0.0018m²/a

Fracture Geometry

PropertyValue
Fracture spacing (2H1)0.05 m
Fracture aperture (2h1)10 μm

These closely spaced fractures create highly efficient lateral pathways for contaminant migration.


Matrix Properties

PropertyValue
Matrix porosity (nm)0.05
Distribution coefficient (Km)0 cm³/g
Dry density2 g/cm³

With no sorption, the matrix acts purely as a diffusive sink, not a reactive barrier.


Domain and Simulation Setup

PropertyValue
Fractured rock thickness (HT)50 m
Number of sub-layers5
Source concentration (co)1
Half-life100 years
Simulation time30 years
Distance of interest50 m

Special Feature: Maximum Sublayer Thickness

This example highlights a POLLUTEv10 special feature:

  • Ability to define sublayers thicker than the default 5 units
  • Allows efficient modeling of large domains (50 m) with fewer layers
  • Maintains numerical stability while improving computational efficiency

This is especially useful in regional-scale fractured rock simulations.


Transport Processes Explained

1. Advective–Dispersive Flow in Fractures

  • Advection drives the contaminant forward along fractures
  • Dispersion spreads the plume longitudinally
  • Results in rapid lateral migration over tens of meters

2. Matrix Diffusion

  • Contaminants diffuse from fractures into the rock matrix
  • Acts as a temporary storage mechanism
  • Slows peak concentrations in fractures
  • Leads to long-term back-diffusion

3. Radioactive Decay

  • Reduces total contaminant mass over time
  • Less significant over 30 years due to long half-life (100 years)
  • Becomes more important in long-term (>100 year) simulations

Graphical Output: Depth vs Concentration


PDF Report

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Engineering and Environmental Insights

  • Fractured rock systems can enable fast contaminant migration, even with low matrix permeability
  • Matrix diffusion is critical for realistic long-term predictions
  • Radioactive decay alone is insufficient for short-term attenuation
  • This type of modeling is essential for:
    • Nuclear waste repository design
    • Risk assessment of radioactive contaminants
    • Long-term groundwater protection strategies

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