Flow factor of non‐continuum fluids in one‐dimensional contact

Emerald - Tập 58 Số 3 - Trang 151-169 - 2006
Y. Zhang1
1Shanxi Institute of Technology, Taiyuan, People's Republic of China

Tóm tắt

PurposeTo develop a more realistic model for molecularly thin film hydrodynamic lubrication by incorporating the fluid inhomogeneity and discontinuity effects across the fluid film thickness in this lubrication.Design/methodology/approachThe total mass flow of the fluid through the contact in a basic one‐dimensional molecularly thin film hydrodynamic lubrication is studied by incorporating the fluid inhomogeneity and discontinuity effects across the fluid film thickness, based on a simplified momentum transfer model between neighboring fluid molecules across the fluid film thickness. This flow is calculated according to the present approach and the theory of viscous flow between two contact surfaces. The total mass flow of the fluid through the contact in this lubrication is also calculated from conventional hydrodynamic lubrication theory, which was based on continuum fluid assumption in the whole lubricated contact. The ratio of this flow calculated from the present approach to that calculated from conventional hydrodynamic lubrication theory is here defined as the flow factor for a one‐dimensional molecularly thin film hydrodynamic lubrication due to the fluid inhomogeneity and discontinuity effects. Results of this flow factor are presented for wide operational parameters.FindingsIn the molecularly thin film hydrodynamic lubrication, when the fluid inhomogeneity and discontinuity across the fluid film thickness both are incorporated, the total fluid mass flow through the contact and thus the global fluid film thickness are increased. The combined effect of the fluid inhomogeneity and discontinuity across the fluid film thickness on the total fluid mass flow through the contact in this lubrication is determined by the operational parameter K=((∂p/∂xh2)/[6ηbulk(1−ξ)(ua+ub)]); when the operational parameter K is high, this effect is significant; when the operational parameter K is low, this effect is negligible. On the other hand, in this lubrication, when the combined effect of the fluid inhomogeneity and discontinuity across the fluid film thickness is incorporated, the shear stresses at the contact‐fluid interfaces are reduced and this reduction can be significant. This reduction may strongly depend on the value of the dimensionless discontinuity parameter Δ/D of the fluid across the fluid film thickness but weakly depend on the number n of the fluid molecules across the fluid film thickness.Practical implicationsAn important and very useful research for the academic researcher and the engineer who are, respectively, engaged in the study and design of hydrodynamic lubrication on mechanical components especially of very low hydrodynamic lubrication film thickness. It is also important to the subsequent research of molecularly thin film hydrodynamic lubrication.Originality/valueA new model of molecularly thin film hydrodynamic lubrication in one‐dimensional contacts is originally proposed and described by incorporating the fluid inhomogeneity and discontinuity effects across the fluid film thickness in this lubrication. This new model of molecularly thin film hydrodynamic lubrication is of importance to the theoretical study of molecularly thin film hydrodynamic lubrication.

Tài liệu tham khảo

Breuer, K.S. (2002), “Lubrication in MEMS”, in Gad‐el‐Hak, M. (Ed.), CRC Handbook on MEMS, CRC Press, Boca Raton, FL. Dowson, D. and Higginson, G.R. (1966), Elastohydrodynamic Lubrication, Pergamon Press, New York, NY. Ehret, P., Dowson, D. and Taylor, C.M. (1998), “On lubricant transport conditions in elastohydrodynamic conjunctions”, Proc. Roy. Soc. Lond., Vol. A454, pp. 763‐87. Haile, J.M. (1997), Molecular Dynamics Simulation, Wiley, New York, NY. Israelachvili, J. (1991), Intermolecular & Surface Forces, Academic Press, New York, NY. Jang, S. and Tichy, J. (1995), “Rheological models for thin film EHL contacts”, ASME Jour. of Trib., Vol. 117, pp. 22‐8. Johnston, G.J., Wayte, R. and Spikes, H.A. (1991), “The measurement and study of very thin lubricant films in concentrated contacts”, Trib. Trans., Vol. 34, pp. 187‐94. Luengo, G., Schmitt, F‐J. and Israelachvili, J. (1997), Macromolecules, Vol. 30, pp. 2482‐94. Matsuoka, H. and Kato, T. (1997), “An ultrathin liquid film lubrication theory‐ calculation method of solvation pressure and its application to the EHL problem”, ASME Jour. of Trib., Vol. 119, pp. 217‐26. Meyer, E., Overney, R.M., Dransfeld, K. and Gyalog, T. (1998), Nanoscience‐Friction and Rheology on the Nanometer Scale, World Scientific Press, River edge, NJ. Pinkus, O. and Sternlicht, B. (1961), Theory of Hydrodynamic Lubrication, McGraw‐Hill, New York, NY. Salomon, G. (1976), “Failure criteria in thin film lubrication – the IRG program”, Wear, Vol. 36, pp. 1‐6. Tichy, J.A. (1995a), “A porous media model for thin film lubrication”, ASME Jour. of Trib., Vol. 117, pp. 16‐21. Tichy, J.A. (1995b), “A surface layer model for thin film lubrication”, Trib. Trans., Vol. 38, pp. 577‐82. Zhang, Y. (2004), “Mixed rheologies in elastohydrodynamic lubrication”, Ind. Lubri. & Trib., Vol. 56, pp. 88‐106.