By Gould R.F. (ed.)

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In the usual theory of solutions in which the number of moles of the two substances is a given quantity, the temperature of curve 1 would fall in the region in which the solution segregated into two phases, one rich in one component, the other rich in the other. The constructions of Fig. 1t is always possible to find a point through which the straight line passes but which does not change with temperature provided r is independent of temperature. The construction is shown in Fig. 1S/kB). [Refs.

88 894 (1966). K. E. SHULER, J. Chem. Phys .. 20 1865 (1952). c. A. BOEYENS, J. Phys. , 71 2969 (1967). A. W. LAWSON, Prog. Metal Phys. 6 1 (1956). D. ADLER in Solid State Physics, Vol. 21, edited by F. SEITZ, D. TURNBULL and H. EHRENREICH, Academic Press, New York (1968). 32. N. F. MOTT, Proc. Phys. Soc. (London) A62 416 (1949). 33. N. F. MOTT, Comments on Solid State Physics II, 183 (1970). 1. CHAPTER THREE Thermal Versus Optical Transitions A common technique for measuring the difference in energy between the ground state and an excited electronic state is by optical absorption which, of course, gives a measure of this difference, subject to definite restrictions.

The first term represents the contribution from the free energy difference at zero pressure, the second term is due to the fact that the two components have different volumes, and the third term is the result of differing bulk moduli. One sees that if one component has a larger volume, but also a larger compressibility (smaller B), the possibility of a maximum in In K versus pressure exists. 11 ) = - [Refs. on p. 59] Ax(1 - 2x). 1). It is not surprising that these equations give only a very qualitative approximation to experiment, as we have neglected r and because it is well known that in the pressure range necessary for these conversions B is definitely dependent on pressure.

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