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(a) t =0
(b) t =9 . 937 · 10 5
(c) t =2 . 291 · 10 3
Fig. 2. Transient solution to the Cahn-Hilliard problem in two spatial dimensions,
subject to a random initial condition and periodic boundary conditions. The weak
form is discretized in space by a mesh of 128 2 C 1 -quadratic elements. The initially
mixed fluid phase-separates.
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