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Chapter VIII Micro-hardness studies…<br />

The first order elastic stiffness constant (C11) has been evaluated for pure<br />

and amino acid doped KDP crystals using Wooster’s empirical relation [65] as<br />

follow:<br />

log C11 = (7/4) log Hv (8.7)<br />

Where, Hv is micro-hardness. The values of C11 are tabulated in table (8.2).<br />

This supports the concept of Onitsch [66], that if n < 2 the micro-<br />

hardness number decreases as the load increases. In low-load regions the<br />

resistance offered by material may be comparable with the applied load,<br />

resulting in a higher value of hardness. However, at higher load the plastic<br />

flow of the material may be higher and hence the resistance offered by the<br />

material is negligible, thus the value of hardness decreases with increase in<br />

the value of applied load.<br />

8.5 Study of Mayer's law or Kick's law:<br />

Variation of micro-hardness with applied load is usually explained for<br />

spherical indenter by Meyer's law [6] and pyramidal indenter by Kick's law<br />

[13]. Later on Kick's law was modified by Hay and Kendall [14], which is<br />

discussed in next section of this chapter. For pyramidal indenter Kick's law is<br />

given as,<br />

P = ad n<br />

301<br />

(8.8)<br />

Where, P is the applied load in gram (or Newton), d is the observed diagonal<br />

length of indentation mark, and n is the constant for a given material. Kick<br />

postulated a constant value of n= 2 for all the indenters and for all<br />

geometrically similar impressions. Nevertheless, Kick’s law did not receive<br />

wide acceptance on account of the fact that n usually has a value less than 2,<br />

particularly in the low load regions. If n is less than 2, the hardness number<br />

increases with decreasing load, and if n is greater than 2, it decreases as the

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