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TECHNICAL PAPERS

A Review of Recent Approaches for Modeling Solid Third Bodies

[+] Author and Article Information
I. Iordanoff, Y. Berthier, S. Descartes

Laboratoire de Mécanique des Contacts UMR INSA-CNRS 5514, 20 Avenue Albert Einstein, 69621 Villeurbanne Cedex

H. Heshmat

Mohawk Innovative Technology, Inc., 1037 Watervliet-Shaker Road, Albany, NY 12205-3833

J. Tribol 124(4), 725-735 (Sep 24, 2002) (11 pages) doi:10.1115/1.1467632 History: Received September 19, 2000; Revised September 25, 2001; Online September 24, 2002
Copyright © 2002 by ASME
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References

Figures

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Velocity accommodation mechanism
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Mode S2Mj (sliding) and S3M3 (shearing) for powder lubricated journal bearing: (a) initial position for sectors of powder; and (b) sectors of powder after 10 cycles
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S3M4 velocity accommodation with SiC
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S3M2 velocity accommodation with MoS2
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M3 and M4 accommodation for SiC
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Qualitative flows evolution during contact life, influence of humidity: (a) dry atmosphere at 24°C; and (b) wet atmosphere at 24°C
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Rheological law for sand (Hou et al. 26)
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Rheological law for a given pressure
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Geometry and nomenclature of a powder film
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Powder-lubricated multi-pad journal bearing and pressure profiles on pad for various eccentricity ratios with powder MoS2
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Quasi-solid behavior for TiO2 rutile powder with grain diameter of 100 nm: (a) influence of shear rate on shear stress; and (b) influence of shear strains on shear stress
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Quasi-hydrodynamic behavior for TiO2 rutile powder with grain diameter of 2 μM
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Experimental device used for I. Iordanoff experiments
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Experimental device used for H. Heshmat experiments
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Influence of the interface on the value of the limiting shear stress
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Plane first body surface after test: (a) rough surface after test; (b) smooth surface after test; and (c) gold surface after test
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Description of the different velocity accommodation modes: (a) velocity accommodation for rough surface; and (b) velocity accommodation for smooth surface with natural or artificial coating
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Building of a macroscopical simulation
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Influence of third body thickness on slipping at wall: (a) slipping at wall for low third body thickness; and (b) velocity repartition for high third body thickness
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Influence of a bridge formation on the instantaneous coefficient of friction
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Spherical particle shape and elongated particle shape
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Building of a granular simulation
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Field of validity for continuum and discrete approach
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Solid behavior obtained with the granular model

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