Apparent molar heat capacities and apparent molar volumes of Y-2(SO4)(3)(aq), La-2(SO4)(3)(aq), Pr-2(SO4)(3)(aq), Nd-2(SO4)(3)(aq),Eu-2(SO4)(3)(aq), Dy-2(SO4)(3)(aq), Ho-2(SO4)(3)(aq), and Lu-2(SO4)(3)(aq) at T=298.15 K and p=0.1 MPa
Ra. Marriott et al., Apparent molar heat capacities and apparent molar volumes of Y-2(SO4)(3)(aq), La-2(SO4)(3)(aq), Pr-2(SO4)(3)(aq), Nd-2(SO4)(3)(aq),Eu-2(SO4)(3)(aq), Dy-2(SO4)(3)(aq), Ho-2(SO4)(3)(aq), and Lu-2(SO4)(3)(aq) at T=298.15 K and p=0.1 MPa, J CHEM THER, 33(6), 2001, pp. 643-687
The apparent molar heat capacities C degrees (p,phi) and apparent molar vol
umes V degrees (phi) of Y-2(SO4)(3)(aq), La-2(SO4)(3)(aq), Pr-2(SO4)(3)(aq)
, Nd-2(SO4)(3)(aq), Eu-2(SO4)(3)(aq), Dy-2(SO4)(3)(aq), Ho-2(SO4)(3)(aq), a
nd Lu-2(SO4)(3)(aq) were measured at T = 298.15 K and p = 0.1 MPa with a So
dev (Picker) flow microcalorimeter and a Sodev vibrating-tube densimeter, r
espectively. These measurements extend from lower molalities of m = (0.005
to 0.018) mol . kg(-1) to m = (0.025 to 0.434) mol . kg(-1), where the uppe
r molality limits are slightly below those of the saturated solutions. Ther
e are no previously published apparent molar heat capacities for these syst
ems, and only limited apparent molar volume information. Considerable amoun
ts of the RSO4+(aq) and R(SO4)(2)(-)(aq) complexes are present, where R den
otes a rare-earth, which complicates the interpretation of these thermodyna
mic quantities. Values of the ionic molar heat capacities and ionic molar v
olumes of these complexes at infinite dilution are derived from the experim
ental information, but the calculations are necessarily quite approximate b
ecause of the need to estimate ionic activity coefficients and other thermo
dynamic quantities. Nevertheless, the derived standard ionic molar properti
es for the various RSO4+(aq) and R(SO4)(2)(-)(aq) complexes are probably re
alistic approximations to the actual values. Comparisons indicate that V de
grees (phi){RSO4+ aq, 298.15 K} = -(6 +/-4)cm(3). mol(-1) and V(phi)degrees
{R(SO4)(2)(-), aq, 298.15 K} = (35 +/-3) cm(3). mol(-1), with no significa
nt variation with rare-earth. In contrast, values of C degrees (p,phi){RSO4
+, aq, 298.15 K} generally increase with the atomic number of the rare-eart
h, whereas C degrees (p,phi){R(SO4)(2)(-), aq, 298.15 K} shows a less regul
ar trend, although its values are always positive and tend to be larger for
the heavier than for the light rare earths. (C) 2001 Academic Press.