Porous Media 1979
DOI: 10.1016/b978-0-12-223650-1.50008-5
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Pore Structure

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Cited by 294 publications
(196 citation statements)
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“…The capillary pressure presents the static force between the non-wetting phase and wetting phase in the porous media and it is an increasing function of the nonwetting phase saturation [29,30].…”
Section: Di-electrical Measurementsmentioning
confidence: 99%
“…The capillary pressure presents the static force between the non-wetting phase and wetting phase in the porous media and it is an increasing function of the nonwetting phase saturation [29,30].…”
Section: Di-electrical Measurementsmentioning
confidence: 99%
“…In a porous material, the molecules are restricted to evolving in the accessible volume: the mean square displacement remains proportional to time, but with an effective diffusion coefficient which is smaller than in bulk. This is because the molecules have to travel a larger distance through tortuous channels [1,2,20].…”
Section: Diffusion Measurementsmentioning
confidence: 99%
“…Both are influenced by the structure and topology of the porous material, as well as the interactions between the fluid molecules and the solid surface. It is important to note that self-diffusion and convection are quite different processes which are not sensitive to the same morphological and topological characteristics of the porous medium [1,2].…”
Section: Introductionmentioning
confidence: 99%
“…The validity of the results were made confirmed by comparing the interfacial area at Str=0 with that of solid surface area. The specific solid surface area was calculated for each porous media assuming that all particles are perfectly spheres and identical in size (Dullien, 1979) and the interfacial area at zero saturation was taken from Fig. 8 by extrapolating the experimental data.…”
Section: Evaluation Of Air-liquid Interfacial Areamentioning
confidence: 99%