Thermodynamics of the cell Pt vertical bar H-2(p)vertical bar HCl (m)vertical bar AgCl vertical bar Ag and primary medium effects upon HCl in (glycerol plus water) solvents
L. Falciola et al., Thermodynamics of the cell Pt vertical bar H-2(p)vertical bar HCl (m)vertical bar AgCl vertical bar Ag and primary medium effects upon HCl in (glycerol plus water) solvents, J CHEM THER, 33(5), 2001, pp. 499-512
The electromotive force (e.m.f.) E of the cell Pt \H-2(p)\ HCl(m) in Z \ Ag
Cl \ Ag in {glycerol (G) + water (W)} solvents, Z = (G + W), up to glycerol
mass fraction w(G) = 0.7 has been measured within the temperature range fr
om 273.15 K to 313.15 K at HCl molalities up to 0.1 mol/kg(-1). On this bas
is, the standard molar e.m.f. E-m(o) values pertaining to such solvent mixt
ures have been obtained, and have been combined with sparse literature data
for optimization. At glycerol mass fractions up to w(G)approximate to0.5,
at constant temperature, E-m(o) shows a linear dependence on the glycerol m
ole fraction X-G and, in parallel, E-c(o) (on the amount-of-substance conce
ntration scale) shows linear dependence on the glycerol volume fraction phi
(G). The primary medium effect upon HCl, defined as the difference (E-c(o)
)w - (E-c(o))Z, has been considered as a function of the water volume fract
ion phi (W) in terms of Feakins and French's theory: this would lead to a p
rimary hydration number n(hydr) = 2.4 for HCl, in good agreement with previ
ous results obtained with solvents other than (glycerol + water). In this c
onnection, some basic methodological aspects are discussed. Ancillary value
s of the densities rho (Z) of the relevant solvent mixtures, which were hit
herto unavailable and are necessary for the data processing leading to E-m(
o), have also been measured. (C) 2001 Academic Press.