P-V-T-x and vapor-liquid equilibrium properties of pentafluoroethane (R125)+1,1,1,3,3,3-hexafluoroethane (R236fa) and 1,1,1,2-tetrafluoroethane (R134a)+R236fa systems derived from isochoric measurements
G. Di Nicola et al., P-V-T-x and vapor-liquid equilibrium properties of pentafluoroethane (R125)+1,1,1,3,3,3-hexafluoroethane (R236fa) and 1,1,1,2-tetrafluoroethane (R134a)+R236fa systems derived from isochoric measurements, J CHEM EN D, 46(2), 2001, pp. 359-366
P-V-T-x measurements were performed using a constant-volume apparatus for t
he pentafluoroethane (R125) + 1,1,1,3,3,3-hexafluoropropane (R236fa) and 1,
1,1,2-tetrafluoroethane (R134a) + 1,1,1,3,3,3-hexafluoropropane (R236fa) sy
stems, in a temperature range of (253-372) K and a pressure range of (113-2
360) kPa. Experimental data were collected on three different compositions
for each of the systems. Eight expansion series with a total of 121 data po
ints and nine expansion series with 110 data points were performed, respect
ively, for the R125 + R236fa and R134a + R236fa systems, both within the va
por-liquid equilibrium (VLE) boundary and in the superheated vapor region.
The data in the superheated vapor region were interpreted using tried and t
ested correlating methods for the second and third virial coefficients. The
VLE parameters were derived by applying two methods: (1) The flash method
enabled VLE parameters to be derived directly from P-V-T-z data within the
VLE boundary by applying the Carnahan-Starling-De Santis (CSD) equation of
state (EOS). (2) The dew-point method was based on dew-point evaluation by
interpolating experimental P-T sequences. The resulting dew-point value was
then used to derive VLE parameters, again using the CSD EOS. A comparison
of the results emerging from these two methods, followed by the interpretat
ion of the volumetric properties of the superheated vapor, confirmed their
internal consistency.