E. Wilhelm et al., THERMODYNAMICS OF (1,4-DIFLUOROBENZENE PLUS AN N-ALKANE) AND OF (HEXAFLUOROBENZENE PLUS AN N-ALKANE), Fluid phase equilibria, 110(1-2), 1995, pp. 299-313
Excess molar enthalpies H-E and excess molar volumes V-E have been mea
sured, as a function of mole fraction x(1), at 298.15 K and atmospheri
c pressure for the five liquid mixtures (x(1)1,4-C6H4F2 + x(2)n-ClH2l2), l = 7, 8, 10, 12 and 16. In addition, H-E and excess molar heat ca
pacities C-P(E) at constant pressure have been determined for the two
liquid mixtures (x(1)C(6)F(6) + x(2)n-ClH2l+2), l = 7 and 14, at the s
ame temperature and pressure. The instruments used were flow microcalo
rimeters of the Picker design (the H-E version was equipped with separ
ators) and a vibrating-tube densimeter, respectively. The excess entha
lpies of the five difluorobenzene mixtures are all positive and quite
large; they increase with increasing chain length l of the n-alkane fr
om H-E(X(1) = 0.5)/(J mol(-1))= 1050 for l = 7 to 1359 for l = 16. The
corresponding excess volumes V-E are all positive and also increase w
ith increasing l: V-E(X(1) = 0.5)/(cm(3) mol(-1)) = 0.650 for l = 7 an
d 1.080 for l = 16. Interestingly, the excess enthalpies of the corres
ponding mixtures with hexafluorobenzene are only about 5% larger, wher
eas the excess volumes of (x(1)C(6)F(6) + x(2)n-ClH2l+2) are roughly t
wice as large as those of their counterparts in the series containing
1,4-C6H4F2. Specifically, at 298.15 K H-E(X(1) = 0.5)/(J mol(-1)) = 11
19 for (x(1)C(6)F(6) + x(2) n-C7H16) and 1324 for (x(1)C(6)F(6) + x(2)
n-C14H30), and for the same mixtures V-E(x(1) = 0.5)/(cm(3) mol(-1)) =
1.882 and 2.093, respectively. The excess heat capacities for both sy
stems are negative and of about the same magnitude as the excess heat
capacities of mixtures of fluorobenzene with the same n-alkanes (Roux
et al., 1984): C-P(E)(x(1) = 0.5)/(J K-1 mol(-1)) = -1.18 for (x(1)C(6
)F(6) + x(2)n-C7H16), and -2.25 for (x(1)C(6)F(6) + x(2)n-C14H30). The
curve C-P(E) vs. (x(1) for x(1)C(6)F(6) + x(2)n-C14H30) shows a sort
of ''hump'' for x(1) 0.5, which is presumed to indicate emerging W-sha
pe composition dependence at lower temperatures.