scholarly journals Analysis of a fully discrete finite element method for the phase field model and approximation of its sharp interface limits

2003 ◽  
Vol 73 (246) ◽  
pp. 541-568 ◽  
Author(s):  
Xiaobing Feng ◽  
Andreas Prohl
Keyword(s):  
Finite Element Method ◽  
Finite Element ◽  
Phase Field ◽  
Field Model ◽  
Phase Field Model ◽  
Sharp Interface ◽  
Fully Discrete ◽  
Discrete Finite Element ◽  
Element Method

scholarly journals Analysis of Transformation Plasticity in Steel Using a Finite Element Method Coupled with a Phase Field Model

PLoS ONE ◽  
2012 ◽  
Vol 7 (4) ◽  
pp. e35987 ◽  
Author(s):  
Yi-Gil Cho ◽  
Jin-You Kim ◽  
Hoon-Hwe Cho ◽  
Pil-Ryung Cha ◽  
Dong-Woo Suh ◽  
...  
Keyword(s):  
Finite Element Method ◽  
Finite Element ◽  
Phase Field ◽  
Field Model ◽  
Phase Field Model ◽  
Transformation Plasticity ◽  
Element Method

scholarly journals Fully-discrete finite element numerical scheme with decoupling structure and energy stability for the Cahn-Hilliard phase-field model of two-phase incompressible flow system with variable density and viscosity

2021 ◽  
Author(s):  
chuanjun chen ◽  
Xiaofeng Yang
Keyword(s):  
Finite Element ◽  
Phase Field ◽  
Numerical Scheme ◽  
Field Model ◽  
Flow System ◽  
Phase Field Model ◽  
Variable Density ◽  
Two Phase ◽  
Fully Discrete ◽  
Discrete Finite Element

We construct a fully-discrete finite element numerical scheme for the Cahn-Hilliard phase-field model of the two-phase incompressible flow system with variable density and viscosity. The scheme is linear, decoupled, and unconditionally energy stable. Its key idea is to combine the penalty method of the Navier-Stokes equations with the Strang operator splitting method, and introduce several nonlical variables and their ordinary differential equations to process coupled nonlinear terms. The scheme is highly efficient and it only needs to solve a series of completely independent linear elliptic equations at each time step, in which the Cahn-Hilliard equation and the pressure Poisson equation only have constant coefficients. We rigorously prove the unconditional energy stability and solvability of the scheme and carry out numerous accuracy/stability examples and various benchmark numerical simulations in 2D and 3D, including the Rayleigh-Taylor instability and rising/coalescence dynamics of bubbles to demonstrate the effectiveness of the scheme, numerically.

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