In the previous paper (Part I) it was demonstrated by means of field ion microscopy that the measured ratio of divacancy concentration to monovacancy concentration ( c2v c1v) in high purity platinum specimens quenched from 1700 ± 1°C was 0.06 ± 0.02. In the present paper (Part II), a detailed series of quantitative calculations was first performed which showed that this ratio was not affected by specimen storage and electropolishing procedures subsequent to the quench and hence represented c2v c1v at the "freeze-out" temperature (T*). It was then shown that all combinations of the divacancy binding energy (E2vb) and binding entropy (S2vb) which lead to a quenched-in value of c2v c1v equal to 0.06 ± 0.02 for a quench temperature of 1700°C are governed by the linear relationship E2vb = [(0.23 ± 0.03) + 6.17 · 10-2( S2vb k)]eV, where k is Boltzmann's constant. This linear equation implies that the divacancy binding free energy (G2vb) was 0.23 eV at T* = 443.4°C. This value of G2vb, calculated from our experimental data, depends only on a knowledge of the monovacaney migration energy and an approximate value of a frequency factor. The existing tracer diffusion data for platinum were re-examined in terms of a monovacancy and divacancy model in an attempt to decompose G2vb into E2vb and S2vb terms, and it was concluded that the available data are not sufficiently accurate to make this decomposition significant.
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