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We examine the scaling properties of one‐dimensional random walks on media with multifractal diffusivities, which is a simple model for transport in scaling porous media. We find both theoretically and numerically that the anomalous scaling exponent of the walk is d w =2 + K (− 1) where K (− 1) is the scaling exponent of the reciprocal spatially averaged (“dressed”) resistance to diffusion. Since K (− 1) > 0, the walk is subdiffusive; the walkers are effectively trapped in a hierarchy of barriers. The trapping is dominated by contributions from a specific order of singularity associated with a phase transition between anomalous and normal diffusion. We discuss the implications for transport in porous media.
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Lovejoy et al. (1998) studied this question.
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