Numerical Energy Dissipation for Time-Fractional Phase-Field Equations

Abstract

The numerical integration of phase-field equations is a delicate task which needs to recover at the discrete level intrinsic properties of the solution such as energy dissipation and maximum principle. Although the theory of energy dissipation for classical phase field models is well established, the corresponding theory for time-fractional phase-field models is still incomplete. In this article, we study certain nonlocal-in-time energies using the first-order stabilized semi-implicit L1 scheme. In particular, we will establish a discrete fractional energy law and a discrete weighted energy law. The extension for a $(2-\alpha )$-order L1 scalar auxiliary variable scheme will be investigated. Moreover, we demonstrate that the energy bound is preserved for the L1 schemes with nonuniform time steps. Several numerical experiments are carried to verify our theoretical analysis.

References in corpus (1)

• Revisit of Semi-Implicit Schemes for Phase-Field Equations

Cited by in corpus (5)

• The variable-step L1 scheme preserving a compatible energy law for time-fractional Allen-Cahn equation
• Energy Stable L2 Schemes for Time-Fractional Phase-Field Equations
• A decreasing upper bound of energy for time-fractional phase-field equations
• Equivalence between a time-fractional and an integer-order gradient flow: The memory effect reflected in the energy
• Energy stability of variable-step L1-type schemes for time-fractional Cahn-Hilliard model