In this paper we develop a fully nonconforming virtual element method of arbitrary approximation order for the two dimensional Cahn–Hilliard equation. We carry out the error analysis for the semidiscrete (continuous-in-time) scheme and verify the theoretical convergence result via numerical experiments. We present a fully discrete scheme which uses a convex splitting Runge–Kutta method to discretize in the temporal variable alongside the virtual element spatial discretization.
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Dedner et al. (2024) studied this question.
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