The Morse function, Φ(r) = D(e − 2e ), is often used to represent interatomic interactions in investigations of a wide variety of physical phenomena. In view of the wide‐spread use of this function, it is of interest to investigate quantitatively the extent to which experimentally determined anharmonic behavior is exhibited by solids with Morse function interatomic interactions. Numerical values of the Morse parameters D, α, and r0 are determined for a number of cubic metals from experimental values of the lattice constant and the elastic moduli C11 and C12. Morse parameters are then used to compute theoretical pressure‐volume (P‐V) behavior, and comparisons are made with P‐V data determined from shock‐wave measurements. Prior studies by other authors have indicated that the Morse function representation of anharmonic effects in metals is satisfactory; however, the present study shows that this representation, in general, becomes fairly poor for pressures which are large enough to produce considerable non‐linearity in the experimentally determined P‐V behavior.
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F. Milstein (1971) studied this question.
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