This paper describes the analysis of the near-continuum hypersonic flow over a compression ramp using the two-dimensional parallel direct simulation Monte Carlo (DSMC) method. Unstructured and triangular solution-based adaptive mesh depending on the local mean free path is used to improve the resolution of solution for the flow field with highly varying properties. In addition, a freestream parameter is defined to help reduced the cell numbers in the freestream area, resulting in appreciable decrease of the computational time (20–30%) without sacrificing the accuracy of the solution. The two-step multilevel graph partition technique is used for physical domain decomposition, employing estimated particle number distribution in each cell as the graph vertex weight. 32 IBM-SP2 processors are used throughout the study unless otherwise specified. The Effect of the outflow vacuum boundary condition, compression ramp angle, freestream condition, and length of the ramp to the flow field are investigated. Computational results are compared with previous numerical results whenever available.

1.
Anderson, J. D., Jr., 1989, Hypersonic and High Temperature Gas Dynamics, McGraw-Hill, New York.
2.
Pullin
,
D. I.
, and
Harvey
,
J. H.
,
1976
, “
A Numerical Simulation of the Rarefied Hypersonic Flat Plate Problem
,”
J. Fluid Mech.
,
78
, pp.
689
707
.
3.
Vogenitz, F. W., Broadwell, J. E., and Bird, G. A., 1969, “Leading Edge Flow by the Monte Carlo Direct Simulation Technique,” 7th Aerospace Science Meeting, AIAA Paper No. 69–141.
4.
Chun, C.-H., 1991, “Experiments on Separation at a Compression Corner in Rarefied Hypersonic Flow,” Rarefied Gas Dynamics, A. Beylich, ed., VCH Publishers, New York, pp. 562–569.
5.
Moss, J., Rault, N., and Price, J. M., 1994, “Direct Monte Carlo Simulations of Hypersonic Viscous Interactions Including Separation,” Rarefied Gas Dynamics: Space Science and Engineering, B. D. Shzgal and D. P. Weave, eds., Washington, DC.
6.
Moss, J. N., Price, J. M., and Chun, C. H., 1991, “Hypersonic Rarefied Flow About a Compression Corner—DSMC Simulation and Experiment,” 26th Thermophysics Conference, AIAA Paper No. 91-1313.
7.
Bird, G. A., 1994, Molecular Gas Dynamics and the Direct Simulation of Gas Flows, Oxford University Press, New York.
8.
Robinson, C. D., 1998, “Particle Simulation on Parallel Computers With Dynamic Load Balancing,” Ph.D. thesis, Imperial College of Science, Technology and Medicine, U.K.
9.
Wu
,
J.-S.
,
Tseng
,
K.-C.
, and
Kuo
,
C.-H.
, 2001, “The Direct Simulation Monte Carlo Method Using Unstructured Adaptive Mesh and Its Application,” Int. J. Numer. Methods Fluids, accepted for publication.
10.
Wu
,
J.-S.
,
Tseng
,
K.-C.
, and
Yang
,
T.-J.
, 2001, “Parallel Implementation of the Direct Simulation Monte Carlo Method Using Unstructured Mesh and Its Application,” Int. J. Numer. Methods Heat Fluid Flow, submitted for publication.
11.
Hypermesh, Version 2.0, Altair Computing, Altair Engineering, Inc., Maplelawn, MI.
12.
Walshaw, C., Cross, M., Everett, M. G., Johnson, S., and McManus, K., 1995, “Partitioning and Mapping of Unstructured Meshes to Parallel Machine Topologies,” Proc. Irregular Parallel Algorithms for Irregularly Structured Problems, A. Ferreia and J. Rolim, eds., 980, LNCS, Springer, Berlin, pp. 121–126.
You do not currently have access to this content.