Hostname: page-component-78c5997874-m6dg7 Total loading time: 0 Render date: 2024-11-17T22:18:43.155Z Has data issue: false hasContentIssue false
  • English
  • Français

Model Simulation of Powder Compaction by Complex Mold Based on Deformation Behavior of Free Particles Measured by Compression Test

Published online by Cambridge University Press:  11 February 2011

Hitoshi Hashimoto ,
Zheng Ming Sun ,
Yong Ho Park  and
Toshihiko Abe
Hitoshi Hashimoto
Affiliation:
Institute for Strunctural and Engineering Materials, AIST Tohoku, 4–2–1, Nigatake, Miyagino-ku, Sendai, 983–8551, Japan.
Zheng Ming Sun
Affiliation:
Institute for Strunctural and Engineering Materials, AIST Tohoku, 4–2–1, Nigatake, Miyagino-ku, Sendai, 983–8551, Japan.
Yong Ho Park
Affiliation:
Institute for Strunctural and Engineering Materials, AIST Tohoku, 4–2–1, Nigatake, Miyagino-ku, Sendai, 983–8551, Japan.
Toshihiko Abe
Affiliation:
Institute for Strunctural and Engineering Materials, AIST Tohoku, 4–2–1, Nigatake, Miyagino-ku, Sendai, 983–8551, Japan.
Get access

Abstract

Discrete element method (DEM) is one of the excellent procedures for model simulation of behavior of granular assemblies. A two-dimensional DEM simulation of powder compaction by a complex mold was conducted by considering the deformation behavior of individual particles measured by a compression test of free particles. Spherical copper particles were used as a model material in this study. The particles (particle size ranges from 38 to 125microns) were individually compressed between parallel platens to measure compressive load and displacement in the loading direction. From the measured load and displacement data, force-displacement relations at contacts between the particles, and between the particles and mold wall were determined. In the simulation, the two-dimensional complex mold consisting of three stages (upper stage:3-mm wide and 1-mm deep, middle stage:2-mm wide and 1-mm deep, lower stage:1-mm wide and 1-mm deep) was charged with the copper powder consisting of spherical particles with size range of 50 to 200microns and was pressed under four press conditions. Forces at all contacts were calculated by using the determined force-displacement relations and each particle's position was traced by solving equations of motion for each particle. Pressure at each wall of the mold and density distribution in the powder compact were calculated as results of the simulation. It was found that the increase in the pressure at each wall corresponds to the increase in the density of the powder near the wall.

Type
Research Article
Information
MRS Online Proceedings Library (OPL) , Volume 759: Symposium MM – Granular Material-Based Technologies , 2002 , MM2.4
Copyright
Copyright © Materials Research Society 2003

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Haeggblad, H.A., Powder Technol, 67, 127 (1991).Google Scholar
2. Gethin, D.T., Tran, V.D., Lewis, R.W. and Ariffin, A.K., Int. J. Powder Metall, 30, 385 (1994).Google Scholar
3. Kraft, T., Riedel, H., Stingel, P. and Wittig, F., Adv. Eng. Mater., 1, 107 (1999).Google Scholar
4. Coube, O. and Riedel, H., Powder Metall, 43, 123 (2000).Google Scholar
5. Cundall, P.A. and Strack, O.D.L.,, Geotechnique, 29, 47 (1979).Google Scholar
6. Kitahara, H., Kotera, H. and Shima, S., Powder Technol, 109, 234 (2000).Google Scholar
7. Redanz, P. and Fleck, N. A., Acta Mater., 49, 4325 (2001).Google Scholar
8. Liu, L. and Yuan, Y., J. Mater. Sci. Lett., 19, 841 (2000).Google Scholar
9. Timoshenko, S.P. and Goodier, J.N., “Theory of Elasticity”, 3rd ed. (McGraw-Hill Kogakusya, Tokyo, 1970) pp.409–414.Google Scholar