Abstract
I consider fluid flow at the interface between solids with random roughness. For anisotropic roughness, obtained by stretching isotropic roughness in the x-direction by a factor of gamma ^{1/2} and in the y-direction with a factor of gamma ^{-1/2}, I give an argument for why the flow conductivity in the critical junction theory should be proportional to gamma in the x-direction and proportional to 1/gamma in the y-direction.
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