The coarsening dynamics of the Cahn-Hilliard equation with order-parameter-dependent mobility, {λ}({φ}){∝}(1-φ²{)}^{{{α}}}$, is addressed at zero temperature in the Lifshitz-Slyozov limit where the minority phase occupies a vanishingly small volume fraction. Despite the absence of bulk diffusion for {α}{}0, the mean domain size is found to grow as 〈R〉{∝}t^1/(3+α), due to subdiffusive transport of the order parameter through the majority phase. The domain-size distribution is determined explicitly for the physically relevant case {α}=1.
No takes yet. Share an insight, caveat, or question.
Bray et al. (1995) studied this question.
Synapse has enriched 3 closely related papers on similar clinical questions. Consider them for comparative context: