Lubricant film thickness in the partial elastohydrodynamic range was measured as a function of rolling speed in a rolling 4-ball configuration, for four mineral oils, two esters and a polyphenylether covering a viscosity range of 8–360 cs. Film thickness is shown to vary with speed as a power function. At the point where a full elastohydrodynamic film is formed, the product of viscosity and speed is constant for most lubricants. Wear rate w after run-in follows a simple wear law w = Ka where a is the total area of asperity contact and K is a constant characteristic of the lubricant, of the order of 1 μg/inch3 for compounded ester type lubricants rating these as best, and 4 μg/inch3 for ester base stock, 6 μg/inch3 for polyphenylether and 13 μg/inch3 for mineral oil base stock, rating these lubricants progressively poorer in the order given, regarding their wear-preventing ability. A hypothesis regarding size and shape of wear particles is derived, suggesting platelet shaped particles. Limited data appear to confirm an exponential distribution of wear particle diameters with a mean of the order of 10−4 inch. Contributed by the ASLE Technical Committee on Bearings and Bearing Lubrication and presented at the Annual Meeting of the American Society of Lubrication Engineers held in Detroit, Michigan, May, 1963.
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Tallian et al. (1965) studied this question.
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