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Integral representation of hydraulic permeability

Chuan Bi, Miao-Jung Yvonne Ou, Shangyou Zhang

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Source: Crossref

Published: May 6, 2022

DOI: 10.1017/prm.2022.25

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Source abstract

In this paper, we show that the permeability of a porous material (Tartar (1980)) and that of a bubbly fluid (Lipton and Avellaneda. Proc. R. Soc. Edinburgh Sect. A: Math . 114 (1990), 71–79) are limiting cases of the complexified version of the two-fluid models posed in Lipton and Avellaneda ( Proc. R. Soc. Edinburgh Sect. A: Math . 114 (1990), 71–79). We assume the viscosity of the inclusion fluid is zμ1z\mu _1 and the viscosity of the hosting fluid is μ1R+\mu _1\in \mathbb {R}^{+} , zCz\in \mathbb {C} . The proof is carried out by the construction of solutions for large z|z| and small z|z| with an iteration process similar to the one used in Bruno and Leo ( Arch. Ration. Mech. Anal . 121 (1993), 303–338) and Golden and Papanicolaou ( Commun. Math. Phys . 90 (1983), 473–491) and the analytic continuation. Moreover, we also show that for a fixed microstructure, the permeabilities of these three cases share the same integral representation formula (3.17) with different values of contrast parameter s:=1/(z1)s:=1/(z-1) , as long as ss is outside the interval [2E221+2E22,11+2E12]\left [-\frac {2E_2^{2}}{1+2E_2^{2}},-\frac {1}{1+2E_1^{2}}\right ] , where the positive constants E1E_1 and E2E_2 are the extension constants that depend only on the geometry of the periodic pore space of the material.

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Integral representation of hydraulic permeability — Mathematical Frontier Network