1987 Volume 1987 Issue 2 Pages 131-139
Regarding the standard entropy and enthalpy of solution of gaseous solutes in solvents, δS°s and δH°s, Abraham's linear equations are examined to clarify the significance of th e solute parameter RHS, and the solvent parameters. On the basis of a previous work on ionic hydration, J. Phys. Soc. Jpn.55, 1021(1986), an effective solute radius re=2rsw(δS°s, m/δS°cw)1/2 is introduced after discussing the correlation between δS°sx. and the square of the van der Waals b radius rb. Here the subscripts m and x of δS°s denote the scale of molality and of mole fraction, δS°cx is the standard entropy of condensation of water vapor, -118.8, J.mol-1.K-1 at 298 K, and rsw is the Stokes radius of water, 1.07×10-8cm at 298 K. It is found out that re2 just equals 2 RHS. The effective area re2 can be extensively used in nonaqueous solvents. Referring to solutes and solvents treated by Abraham, δS°s, x, δH°s, and the standard Gibbs energy of solution δG°sx can be expressed as linear, equations of re2, with coefficients BS and BH and constant terms AS and AH characteristic of solvents. Effec tive solute radii re.o at δG°s, x=0 are calculated for 28 solvents by using individual values of AH, AS, BH, and BS. For water alone, there is no real value of re.o. For 27 nonaqueous solven ts, the averaged value of re.o is (2.56±0.20)×10-8 cm, by which an averaged nonaqueous solvent is discussed. An excess amount of δG°s, x, for water from that for the averaged nonaqueous solvent is attributed to the hydrophobic hydration of solutes.
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