No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Direct simulation Monte Carlo method for an arbitrary intermolecular potential
1. G. A. Bird, Molecular Gas Dynamics and the Direct Simulation of Gas Flows (Oxford University Press, Oxford, 1994).
2. M. S. Ivanov, S. F. Gimelshein, and A. E. Beylich, “Hysteresis effect in stationary reflection of shock waves,” Phys. Fluids 7, 685 (1995).
4. K. Koura, H. Matsumoto, and T. Shimada, “A test of equivalence of the variable-hard-sphere and inverse-power-law models in the direct-simulation Monte-Carlo method,” Phys. Fluids 3, 1835 (1991).
6. H. Matsumotoa, “Variable sphere molecular model for inverse power law and Lennard-Jones potentials in Monte Carlo simulations,” Phys. Fluids 14, 4256 (2002).
8. J. Kestin, K. Knierim, E. A. Mason, B. Najafi, S. T. Ro, and M. Waldman, “Equilibrium and transport properties of the noble gases and their mixture at low densities,” J. Phys. Chem. Ref. Data 13, 229 (1984).
9. J. O. Hirschfelder, C. F. Curtiss, and R. B. Bird, The Molecular Theory of Gases and Liquids (Wiley, New York, 1954).
10. F. Sharipov and G. Bertoldo, “Numerical solution of the linearized Boltzmann equation for an arbitrary intermolecular potential,” J. Comput. Phys. 228, 3345 (2009).
11. F. Sharipov, “Data on the velocity slip and temperature jump on a gas-solid interface,” J. Phys. Chem. Ref. Data 40, 023101 (2011).
14. M. Wakabayashi, T. Ohwada, and F. Golse, “Numerical analysis of the shear and thermal creep flows of a rarefied gas over the plane wall of a Maxwell-type boundary on the basis of the linearized Boltzmann equation for hard-sphere molecules,” Eur. J. Mech. B/Fluids 15, 175 (1996).
Article metrics loading...
Full text loading...
Most read this month