Chemistry Reference
In-Depth Information
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Reduced Bulk Density
FIGURE 8.4 Solvent density dependence of V 2 (SR) and H r ,∞ (SR) for the attractive Lennard-
Jones pyrene (2)/CO 2 (1) system along the near-critical reduced isotherm T r = 1.02. All quanti-
ties are made dimensionless using the solvent's Lennard-Jones parameters from Table 8.1.
regression purposes, for example, to estimate accurate values of V 2 at other supercrit-
ical state conditions (Gruszkiewicz and Wood 1997) based only on the corresponding
water properties, but it also suggested some relevant questions regarding the micro-
scopic mechanism underlying such a behavior for D 21 ( T ,ρ).
To gain insights into the observed behavior of D 21 ( T ,ρ), we carried out integral
equation (IE) calculations on model systems defined as charged hard-sphere ions
immersed in an aqueous-like solvent, described as hard spheres with embedded
point polarizabilities and permanent electrostatic multipole moments including
quadrupole and octupoles, by solving the reference hypernetted-chain (RHNC)
equations with solvent polarization effects treated at the self-consistent mean-
field (SCMF) level (Chialvo and Cummings 1994, 1999; Chialvo et al. 2000c). In
Figure 8.10, we display the IE-predicted solvent density dependence of D 21 ( T ,ρ)
along three supercritical isotherms for infinitely dilute CsBr aqueous-like solu-
tions (Chialvo et al. 2001), in comparison with the corresponding experimental
data from Sedlbauer, Yezdimer, and Wood (1998) within the temperature and
density ranges 604 < T(K) < 717 and 0.26 < ρ (g/ cm 3 ) < 0.60, respectively. The
outstanding feature of the IE results is their lack of temperature dependence for
supercritical densities, that is, D 21 ( T ,ρ) ≅ D 21 (ρ ≥ ρ c ), a behavior that mirrors the
experimental observations in other supercritical aqueous electrolyte and nonelec-
trolyte systems (O'Connell, Sharygin, and Wood 1996; Gruszkiewicz and Wood
1997; Sedlbauer, Yezdimer, and Wood 1998).
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