A modular particle-continuum (MPC) numerical method for steady-state flows is presented which solves the Navier-Stokes equations in regions of near-equilibrium and uses the direct simulation Monte Carlo (DSMC) method to simulate regions of non-equilibrium gas flow. Existing, state-of-the-art, DSMC a
A Method for Near-Equilibrium Discrete-Velocity Gas Flows
β Scribed by B.T. Nadiga; D.I. Pullin
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 516 KB
- Volume
- 112
- Category
- Article
- ISSN
- 0021-9991
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β¦ Synopsis
We present a simulation scheme for discrete-velocity gases based on local thermodynamic equilibrium. Exploting the kinetic nature of discrete-velocity gases, in that context, results in a natural splitting of fluxes, and the resultant scheme strongly resembles the original process. The kinetic nature of the scheme and the modeling of the infinite collision rate limit, result in a small value of the coefficient of (numerical)-viscosity, the behavior of which is remarkably physical. A first-order method and two second-order methods using the total variation diminishing principle are developed and an example application is presented. Given the same computer resources, it is expected that with this approach, a much higher Reynold's number will be achievable than presently possible with either lattice gas automata or lattice Boltzmann approaches. The ideas being general, the scheme is applicable to any discrete-velocity model and to lattice gases as well. (C) 1994 Academic Press, Inc.
π SIMILAR VOLUMES
In this paper we consider a variety of schemes for performing interpolation in space and time to allow particle trajectories to be integrated from a velocity field given only on a discrete collection of data points in space and time. Using a widely-studied model of chaotic advection as a test case w
The relation between the lattice Boltzmann method, which has recently become popular, and the kinetic schemes, which are routinely used in computational fluid dynamics, is explored. A new discrete velocity method for the numerical solution of Navier-Stokes equations for incompressible fluid flow is