Abstract
IT was found by Meyer1 that when a hard ball is pressed into the surface of a metal by a force F, thus forming an impression of diameter d, the relation holds, where k is a constant depending upon the metal and ball diameter and n, the Meyer index, is a constant depending only upon the metal. The Meyer index is 2.0 for metals which do not work-harden, for example, materials already fully worked, whereas for materials which do work-harden n is greater than 2.0, the greatest value being about 2.5. It has so far only been possible to examine equation (1) under conditions of static loading, but recently a method has been described for the continuous measurement of force throughout impact2, and this has been adapted for the measurement of the index n under dynamic conditions. The force used for this purpose is the maximum force of impact, and the diameter is the diameter of the impression left after impact.
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References
Meyer, E., Z VDI, 645, 740, 835 (1908). See also Tabor, D., “The Hardness of Metals” (Oxf. Univ. Press, 1951).
Crook, A. W., Proc. Roy. Soc., A, 212, 377 (1952).
Finniston, H. M., Jones, E. R. W., and Madsen, P. E., Nature, 164, 1128 (1949).
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CROOK, A. Work-hardening of Annealed Mild Steel under Static and Dynamic Conditions. Nature 170, 1124–1125 (1952). https://doi.org/10.1038/1701124a0
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DOI: https://doi.org/10.1038/1701124a0
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