A mixed Brownian dynamics - SPH method for the simulation of flows of suspensions of bead-spring chains in confined geometries with hydrodynamic interaction

被引:3
作者
Noutcheuwa, Rodrigue Keou [2 ]
Owens, Robert G. [1 ]
机构
[1] Univ Montreal, Dept Math & Stat, Montreal, PQ H3C 3J7, Canada
[2] Univ Montreal, Dept Phys, Montreal, PQ H3C 3J7, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
Brownian dynamics; Smoothed particle hydrodynamics; Hydrodynamic interactions; Fluctuating hydrodynamics; Coupled Langevin equations; Confined flows; SMOOTHED PARTICLE HYDRODYNAMICS; IMMERSED BOUNDARY METHOD; DILUTE POLYMER-SOLUTIONS; NAVIER-STOKES EQUATIONS; LOW-REYNOLDS-NUMBER; DIFFUSION EQUATION; LATTICE BOLTZMANN; STOCHASTIC SIMULATIONS; INCOMPRESSIBLE FLOWS; PROJECTION METHODS;
D O I
10.1016/j.jnnfm.2011.08.011
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
A new coupled Brownian dynamics-smoothed particle hydrodynamics method for the computation of confined flows of non-dilute polymer solutions with full hydrodynamic interaction and excluded volume forces is presented. The starting point for the algorithm is the system of coupled Langevin equations for polymer and solvent (CLEPS) (see Oono and Freed (1981) and Ottinger and Rabin (1989), for example) describing, in the present case, the microscopic dynamics of a flowing polymer solution with a bead-spring representation of the macromolecules. Of crucial importance to the success of our numerical scheme is the manner in which bead forces are transmitted to the fluid. We adopt an approach which is reminiscent of the method of regularized Stokeslets (Cortez, 2001). Numerical tests of some two-dimensional channel flows reveal that use of a second-order projection scheme coupled with fixed SPH quadrature points leads to second-order velocity convergence and almost second-order pressure convergence, provided that the solution is sufficiently smooth. In the case of large-scale dumbbell and bead-spring chain calculations, an appropriate scaling of the number of grid points as a function of the number of beads N ensures, in the absence of excluded volume forces, that the cost of our algorithm is O(N) flops. (C) 2011 Elsevier B.V. All rights reserved.
引用
收藏
页码:1327 / 1346
页数:20
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