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Percolative transport in fractal porous media

✍ Scribed by A.G. Hunt


Publisher
Elsevier Science
Year
2004
Tongue
English
Weight
216 KB
Volume
19
Category
Article
ISSN
0960-0779

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✦ Synopsis


Application of continuum percolation theory to a fractal pore space model yields results for the constitutive relationships for unsaturated flow in agreement with experiment. This application also unites understanding in that the same dry end moisture content, h t ΒΌ 0:039SA 0:52 vol as a function of the surface area to volume ratio, is shown to be associated with the deviation of experimental water retention from fractal scaling as well as with the vanishing of the diffusion constant. Substituted into a critical path analysis (based on continuum percolation theory) for the dependence of the unsaturated hydraulic conductivity, KΓ°hÞ, on moisture, the same value of h t produces excellent agreement with experimental data (y ΒΌ 1:0015x Γ€ 0:0065, R 2 ΒΌ 0:96), with y experiment, x theory and using no adjustable parameters. Though critical path analysis is based on percolation theory, the result obtained for KΓ°hÞ is more closely tied to the fractal characteristics of the medium, and the dependence is referred to as a fractal scaling of the hydraulic conductivity. In all three properties, the interpretation of h t is the same; it represents the minimum value for which a continuous interconnected path of capillary flow is possible, making it the critical volume fraction for percolation. This identification means that the low moisture content deviation from fractal predictions in hΓ°hÞ does not conflict with fractal models of the pore space, as the deviation is due to dynamics rather than to structure. Critical path analysis does not yield percolation scaling, in which K vanishes as a power of Γ°h Γ€ h t Þ. However, it is shown here that the data for KΓ°hÞ and hΓ°hÞ are consistent with an interpretation in which the fractal scaling of K at large moisture contents crosses over to a percolation scaling at a moisture content slightly above h t .


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