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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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5.5 The phenomenological theory <strong>of</strong> solvent effects 303<br />

greater than sucrose-ethanol energies. We may expect that the sucrose-water interfacial<br />

tension is very low.<br />

Now, gA turned out to be negative because gA(γ2-γ1), a positive quantity as generated<br />

by eq. [5.5.23], was divided by (γ2-γ1), a difference <strong>of</strong> surface tensions that is negative. Inevitably<br />

gA was found to be negative. The interfacial tension argument, however, leads to the<br />

conclusion that division should have been by the difference in interfacial tensions. We have<br />

seen that the interfacial tension between sucrose and water may be unusually low. Thus the<br />

factor (γ2-γ1), when replaced by a difference <strong>of</strong> interfacial tensions, namely [γ(sucrose/ethanol)<br />

- γ(sucrose/water)], is <strong>of</strong> uncertain magnitude and sign. We therefore do not know the<br />

sign <strong>of</strong> gA; we only know that the quantity we label gA(γ2-γ1) is positive. This real example<br />

demonstrates the soundness <strong>of</strong> the advice that products <strong>of</strong> the form gAγ not be separated into<br />

their factors. 27,28<br />

5.5.5 NOTES AND REFERENCES<br />

1 D. Khossravi and K.A. Connors, J. Pharm. Sci., 81, 371 (1992).<br />

2 R.R. Pfeiffer, K.S. Yang, and M.A. Tucker, J. Pharm. Sci., 59, 1809 (1970).<br />

3 J.B. Bogardus, J. Pharm. Sci., 72, 837 (1983).<br />

4 P.L. Gould, J.R. Howard, and G.A. Oldershaw, Int. J. Pharm., 51, 195 (1989).<br />

5 Also, when K1 = 1 and K2 = 1, eq. [5.5.13] shows that ΔGsolv = ΔGWW; in this special case the solvation<br />

energy is composition-independent.<br />

6 H.H. Uhlig, J. Phys. Chem., 41, 1215 (1937).<br />

7 J.E. Leffler and E. Grunwald, Rates and Equilibria <strong>of</strong> Organic Reactions, J. Wiley & Sons, New York,<br />

1963, p. 22.<br />

8 J.M. LePree, M.J. Mulski, and K.A. Connors, J. Chem. Soc., Perkin Trans. 2, 1491 (1994).<br />

9 The curvature correction factor g is dimensionless, as are the solvation constants K1 and K2. The parameter<br />

gA is expressed in Å 2 molecule -1 by giving the surface tension the units J Å -2 (where 1 erg cm -2 =1x10 -23 J<br />

Å -2 ).<br />

10 D. Khossravi and K.A. Connors, J. Pharm. Sci., 82, 817 (1993).<br />

11 J.M. LePree, Ph.D. Dissertation, University <strong>of</strong> Wisconsin-Madison, 1995, p. 29.<br />

12 A. Leo, C. Hansch, and D. Elkins, Chem. Revs., 71, 525 (1971).<br />

13 C. Reichardt, <strong>Solvents</strong> and Solvent Effects in Organic Chemistry, VCH, Weinheim, 1988.<br />

14 D. Khossravi and K.A. Connors, J. Solution Chem., 22, 321 (1993).<br />

15 K.A. Connors and J.L. Wright, Anal. Chem., 61, 194 (1989).<br />

16 K.A. Connors, Binding Constants, Wiley-Interscience, New York, 1987, pp. 51, 78.<br />

17 R.D. Skwierczynski and K.A. Connors, J. Chem. Soc., Perkin Trans. 2, 467 (1994).<br />

18 K.A. Connors and D. Khossravi, J. Solution Chem., 22, 677 (1993).<br />

19 M.J. Mulski and K.A. Connors, Supramol, Chem., 4, 271 (1995).<br />

20 K.A. Connors, M.J. Mulski, and A. Paulson, J. Org. Chem., 57, 1794 (1992).<br />

21 J.M. LePree and K.A. Connors, J. Pharm. Sci., 85, 560 (1996).<br />

22 M.C. Brown, J.M. LePree, and K.A. Connors, Int. J. Chem. Kinetics, 28, 791 (1996).<br />

23 J.M. LePree and M.E. Cancino, J. Chromatogr. A, 829, 41 (1998).<br />

24 The validity <strong>of</strong> this approximation can be assessed. The free energy <strong>of</strong> hydration <strong>of</strong> benzene is given as -0.77<br />

kJ mol -1 (E. Grunwald, Thermodynamics <strong>of</strong> Molecular Species, Wiley-Interscience, New York, 1997,<br />

p. 290). Doubling this to -1.5 kJ mol -1 because <strong>of</strong> the greater surface area <strong>of</strong> naphthalene and repeating the<br />

calculation gives g1A1γ1 =4.88x10 -20 J molecule -1 , not sufficiently different from the value given in the text<br />

to change any conclusions.<br />

25 D. Khossravi, Ph.D. Dissertation, University <strong>of</strong> Wisconsin-Madison, 1992, p. 141.<br />

26 F.M. Fowkes, Chemistry and Physics <strong>of</strong> Interfaces; American Chemical Society: Washington, D.C., 1965,<br />

Chap. 1.<br />

27 The introduction <strong>of</strong> the interfacial tension into the cavity term was first done by Yalkowsky et al., 28 who also<br />

argue that a separate solute-solvent interaction term is unneeded, as the solute-solvent interaction is already<br />

embodied in the interfacial tension. In our theory we explicitly show the coupling between the solute-solvent<br />

and solvent-solvent interactions (eq. [5.5.19]), but this is in addition to the solute-solvent interaction (eq.<br />

[5.5.13]). This difference between the two theories is a subtle issue that requires clarification.<br />

28 S.H. Yalkowsky, G.L. Amidon, G. Zografi, and G.L. Flynn, J. Pharm. Sci., 64, 48 (1975).

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