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Work-hardening of Annealed Mild Steel under Static and Dynamic Conditions

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

  1. Meyer, E., Z VDI, 645, 740, 835 (1908). See also Tabor, D., “The Hardness of Metals” (Oxf. Univ. Press, 1951).

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  2. Crook, A. W., Proc. Roy. Soc., A, 212, 377 (1952).

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  3. 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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