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TECHNICAL PAPERS

Extension of the Friction Mastercurve to Limiting Shear Stress Models

[+] Author and Article Information
B. Jacod, C. H. Venner

University of Twente, Faculty of Mechanical Engineering, P.O. Box 217, NL 7500 AE Enschede, The Netherlands

P. M. Lugt

SKF Engineering and Research Center B.V., P.O. Box 2350, NL 3430 DT Nieuwegein, The Netherlands

J. Tribol 125(4), 739-746 (Sep 25, 2003) (8 pages) doi:10.1115/1.1572513 History: Received January 03, 2002; Revised December 30, 2002; Online September 25, 2003
Copyright © 2003 by ASME
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References

Figures

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Rheological models. For the Eyring model τ0L/3.
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Reduced friction coefficient, μ̄, as a function of τ̄c for the circular model, n=2
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Reduced friction coefficient, μ̄, as a function of τ̄c(p*) for the circular model, n=2. Dashed line: Eq. 15.
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Reduced friction coefficient, μ̄, as a function of τ̄c(p*) for the general model, n=1. Dashed line: Eq. 15.
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Reduced friction coefficient, μ̄, as a function of τ̄c(p*) for the general model, n=1.8. Dashed line: Eq. 15
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Reduced friction coefficient, μ̄, as a function of τ̄c(p*) for the Gecim and Winer’s model. Dashed line: Eq. 15.
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Comparison between experimental results plotted as a function of (τ̄c(p*),μ̄) and Eq. 15
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Comparison between experimental results plotted as a function of (τ̄c(p*),μ̄) and Eq. 15. The inlet temperatures have been slightly modified to account for thermal effects.
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Comparison between η̄X/η̄ given by an analytical integration of Eq. 32, Eq. 35 and the relation given in 1. n=2,τ̄m=1−δτ̄.
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Comparison between η̄Y/η̄ given by an analytical integration of Eq. 32, Eq. 35 and the relation given in 1. n=2,τ̄m=1−δτ̄.

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