On anisotropy function in crystal growth simulations using Lattice Boltzmann equation

被引:38
作者
Younsi, Amina [1 ,2 ]
Cartalade, Alain [1 ]
机构
[1] Univ Paris Saclay, CEA, LMSF, STMF,Den DM2S, F-91191 Gif Sur Yvette, France
[2] CS, 22 Ave Galilee, F-92350 Le Plessis Robinson, France
关键词
Lattice Boltzmann method; Phase-field model; Crystal growth; Anisotropy function; Directional derivatives method; PHASE-FIELD MODEL; BINARY-ALLOY SOLIDIFICATION; DENDRITIC GROWTH; NUMERICAL-SIMULATION; PARASITIC CURRENTS; REACTION-DIFFUSION; CUBIC HARMONICS; EXTERNAL FLOWS; DIMENSIONS; WULFF SHAPE;
D O I
10.1016/j.jcp.2016.08.014
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
In this paper, we present the ability of the Lattice Boltzmann (LB) equation, usually applied to simulate fluid flows, to simulate various shapes of crystals. Crystal growth is modeled with a phase-field model for a pure substance, numerically solved with a LB method in 2D and 3D. This study focuses on the anisotropy function that is responsible for the anisotropic surface tension between the solid phase and the liquid phase. The anisotropy function involves the unit normal vectors of the interface, defined by gradients of phase-field. Those gradients have to be consistent with the underlying lattice of the LB method in order to avoid unwanted effects of numerical anisotropy. Isotropy of the solution is obtained when the directional derivatives method, specific for each lattice, is applied for computing the gradient terms. With the central finite differences method, the phase-field does not match with its rotation and the solution is not any more isotropic. Next, the method is applied to simulate simultaneous growth of several crystals, each of them being defined by its own anisotropy function. Finally, various shapes of 3D crystals are simulated with standard and nonstandard anisotropy functions which favor growth in < 100 >-, < 110 >- and < 111 >-directions. (C) 2016 Elsevier Inc. All rights reserved.
引用
收藏
页码:1 / 21
页数:21
相关论文
共 70 条
[1]   A phase-field model of solidification with convection [J].
Anderson, DM ;
McFadden, GB ;
Wheeler, AA .
PHYSICA D-NONLINEAR PHENOMENA, 2000, 135 (1-2) :175-194
[2]  
[Anonymous], 2013, THESIS TONGJI U CHIN
[3]   Phase-field simulation of solidification [J].
Boettinger, WJ ;
Warren, JA ;
Beckermann, C ;
Karma, A .
ANNUAL REVIEW OF MATERIALS RESEARCH, 2002, 32 :163-194
[4]   Three dimensional thermal-solute phase field simulation of binary alloy solidification [J].
Bollada, P. C. ;
Goodyer, C. E. ;
Jimack, P. K. ;
Mullis, A. M. ;
Yang, F. W. .
JOURNAL OF COMPUTATIONAL PHYSICS, 2015, 287 :130-150
[5]   Linking phase-field and atomistic simulations to model dendritic solidification in highly undercooled melts [J].
Bragard, J ;
Karma, A ;
Lee, YH ;
Plapp, M .
INTERFACE SCIENCE, 2002, 10 (2-3) :121-136
[6]  
BRENT AD, 1988, NUMER HEAT TRANSFER, V13, P297, DOI 10.1080/10407788808913615
[7]   Lattice Boltzmann simulations of 3D crystal growth: Numerical schemes for a phase-field model with anti-trapping current [J].
Cartalade, Alain ;
Younsi, Amina ;
Plapp, Mathis .
COMPUTERS & MATHEMATICS WITH APPLICATIONS, 2016, 71 (09) :1784-1798
[8]   Simulations of phase-field models for crystal growth and phase separation [J].
Cartalade, Alain ;
Younsi, Amina ;
Regnier, Elise ;
Schuller, Sophie .
2ND INTERNATIONAL SUMMER SCHOOL ON NUCLEAR GLASS WASTEFORM: STRUCTURE, PROPERTIES AND LONG-TERM BEHAVIOR (SUMGLASS 2013), 2014, 7 :72-78
[9]   A hybrid lattice Boltzmann model for solid-liquid phase transition in presence of fluid flow [J].
Chatterjee, D ;
Chakraborty, S .
PHYSICS LETTERS A, 2006, 351 (4-5) :359-367
[10]   Adaptive phase field simulation of dendritic crystal growth in a forced flow: 2D vs 3D morphologies [J].
Chen, C. C. ;
Tsai, Y. L. ;
Lan, C. W. .
INTERNATIONAL JOURNAL OF HEAT AND MASS TRANSFER, 2009, 52 (5-6) :1158-1166