Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 2. Numerical results

Author:

Ladd Anthony J. C.

Abstract

A new and very general technique for simulating solid–fluid suspensions has been described in a previous paper (Part 1); the most important feature of the new method is that the computational cost scales linearly with the number of particles. In this paper (Part 2), extensive numerical tests of the method are described; results are presented for creeping flows, both with and without Brownian motion, and at finite Reynolds numbers. Hydrodynamic interactions, transport coefficients, and the short-time dynamics of random dispersions of up to 1024 colloidal particles have been simulated.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference30 articles.

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2. Lovalenti, P. M. & Brady, J. F. 1993 The hydrodynamic force on a rigid particle undergoing arbitrary time-dependent motion at small Reynolds number.J. Fluid Mech. 256,561.

3. Ladd, A. J. C. 1994 Numerical simulations of particulate suspensions via a discretized Boltzmann equation. Part 1. Theoretical foundation.J. Fluid Mech. 271,285.

4. Hoover, W. G. , Evans, D. J. , Hickman, R. B. , Ladd, A. J. C. , Ashurst, W. T. & Moran, B. 1980 Lennard–Jones triple-point bulk and shear viscosities. Green–Kubo theory, Hamiltonian mechanics, and nonequilibrium molecular dynamics.Phys. Rev. A22,1690.

5. Hinch, E. J. 1975 Application of the Langevin equation to fluid suspensions.J. Fluid Mech. 72,499.

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