This paper develops a third-order fully decoupled numerical scheme for the hydrodynamically-coupled binary phase-field crystal (BPFC) model based on the relaxed exponential scalar auxiliary variable (E-SAV) approach. The governing equations are derived from the $ L^2 $-gradient flow and coupled with the incompressible Navier-Stokes equations. To preserve total mass conservation, two nonlocal Lagrange multipliers are introduced into the chemical potentials. For temporal discretization, a third-order backward differentiation formula (BDF3) combined with explicit extrapolation techniques is adopted, leading to a linear and fully decoupled time-marching scheme. In addition, a relaxation strategy is incorporated into the E-SAV framework to improve the consistency between the modified energy and the original energy functional. Compared with existing second-order relaxed E-SAV schemes, the proposed method achieves higher temporal accuracy while retaining the advantages of linearity, decoupling, and energy stability. The proposed scheme only requires solving several linear elliptic equations with constant coefficients at each time step, making the algorithm computationally efficient and easy to implement. The unique solvability and discrete energy dissipation property of the numerical scheme are theoretically established. Furthermore, a consistency analysis is provided to show that the relaxation step preserves the third-order temporal accuracy of the primary variables and does not affect the overall convergence order of the scheme. Numerical experiments verify the expected third-order convergence rate, demonstrate the unconditional energy stability of the proposed scheme, and illustrate its effectiveness for long-time simulations of hydrodynamically-coupled crystal growth problems.
Citation: Yue Shen, Wenjie Wang, Xiaoyue Xie. A third-order fully decoupled relaxed E-SAV scheme for the hydrodynamically-coupled binary phase-field crystal model[J]. AIMS Mathematics, 2026, 11(8): 23687-23717. doi: 10.3934/math.2026954
This paper develops a third-order fully decoupled numerical scheme for the hydrodynamically-coupled binary phase-field crystal (BPFC) model based on the relaxed exponential scalar auxiliary variable (E-SAV) approach. The governing equations are derived from the $ L^2 $-gradient flow and coupled with the incompressible Navier-Stokes equations. To preserve total mass conservation, two nonlocal Lagrange multipliers are introduced into the chemical potentials. For temporal discretization, a third-order backward differentiation formula (BDF3) combined with explicit extrapolation techniques is adopted, leading to a linear and fully decoupled time-marching scheme. In addition, a relaxation strategy is incorporated into the E-SAV framework to improve the consistency between the modified energy and the original energy functional. Compared with existing second-order relaxed E-SAV schemes, the proposed method achieves higher temporal accuracy while retaining the advantages of linearity, decoupling, and energy stability. The proposed scheme only requires solving several linear elliptic equations with constant coefficients at each time step, making the algorithm computationally efficient and easy to implement. The unique solvability and discrete energy dissipation property of the numerical scheme are theoretically established. Furthermore, a consistency analysis is provided to show that the relaxation step preserves the third-order temporal accuracy of the primary variables and does not affect the overall convergence order of the scheme. Numerical experiments verify the expected third-order convergence rate, demonstrate the unconditional energy stability of the proposed scheme, and illustrate its effectiveness for long-time simulations of hydrodynamically-coupled crystal growth problems.
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