1994
DOI: 10.1016/0020-7225(94)90050-7
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Similarity of sharp-edged porous media

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Cited by 5 publications
(2 citation statements)
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“…It was shown that α(ω) = α ∞ − [ib(ω)/ωφρ f ]. A thorough theoretical and experimental description of these phenomena was given by Lévy (1979), Auriault (1980), Auriault, Borne & Chambon (1985), Johnson, Koplik & Dashen (1987), Smeulders, Eggels & van Dongen (1992b) and Smeulders et al (1994). The solution of (3.5) and (3.6) is given byv m = A m exp(−ikz), where k is the wavenumber and A m is an arbitrary constant.…”
Section: Plane Wave Propagationmentioning
confidence: 99%
“…It was shown that α(ω) = α ∞ − [ib(ω)/ωφρ f ]. A thorough theoretical and experimental description of these phenomena was given by Lévy (1979), Auriault (1980), Auriault, Borne & Chambon (1985), Johnson, Koplik & Dashen (1987), Smeulders, Eggels & van Dongen (1992b) and Smeulders et al (1994). The solution of (3.5) and (3.6) is given byv m = A m exp(−ikz), where k is the wavenumber and A m is an arbitrary constant.…”
Section: Plane Wave Propagationmentioning
confidence: 99%
“…These morphologies had in common that they were smooth on the pore scale, i.e., the pore surface had bounded curvature. The possibility of departure from the structure function f for corrugated morphologies was investigated by several authors such as Kostek et al, 9 Smeulders et al, 10 Firdaouss et al, 11 and Cortis and Smeulders. 12 It appeared that high values for 1 ϫ 2 could be reached for special cases, but these investigations still did not consider any comparison over the frequency domain.…”
Section: ͑3͒mentioning
confidence: 99%