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The Meyer hardness test is a rarely used hardness test based upon projected area of an impression. This is a more fundamental measurement of hardness than other hardness tests which are based on the surface area of an indentation. The principle behind the test is that the mean pressure required to test the material is the measurement of the hardness of the material. The mean pressure is calculated by dividing the load by the projected area of the indentation. The result is called the Meyer hardness, which has units of megapascals (MPa).〔.〕 An advantage of the Meyer test is that it is less sensitive to the applied load, especially compared to the Brinell hardness test. For cold worked materials the Meyer hardness is relatively constant and independent of load, whereas for the Brinell hardness test it decreases with higher loads. For annealed materials the Meyer hardness increases continuously with load due to strain hardening.〔 Based on Meyer's law hardness values from this test can be converted into Brinell hardness values, and vice versa.〔Tabor, p. 10.〕 The Meyer hardness test was devised by Prof. Eugene Meyer of the Materials Testing Laboratory at the Imperial School of Technology, Charlottenburg, Germany, circa 1908.〔E. Meyer, "Untersuchungen über Härteprüfung und Härte Brinell Methoden," ''Z. Ver. deut. Ing.'', 52 (1908).〕〔V.E. Lysaght, ''Indentation Hardness Testing'', New York: Reinhold Publishing Corp., 1949, p 39-47.〕 ==See also== *Brinelling *Hardness comparison *Knoop hardness test *Leeb Rebound Hardness Test *Rockwell scale *Vickers hardness test 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Meyer hardness test」の詳細全文を読む スポンサード リンク
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