Isochoric heat capacity measurements for 2,2-dichloro-1,1,1-trifluoroethane (R123) at temperatures from 167 to 341 K and 1-chloro-1,2,2,2-tetrafluoroethane (R124) from 94 to 341 K at pressures to 35 MPa
Jw. Magee, Isochoric heat capacity measurements for 2,2-dichloro-1,1,1-trifluoroethane (R123) at temperatures from 167 to 341 K and 1-chloro-1,2,2,2-tetrafluoroethane (R124) from 94 to 341 K at pressures to 35 MPa, INT J THERM, 21(6), 2000, pp. 1303-1320
Molar hear capacities at a constant volume (C-v) of 2,2-dichloro-1,1,1-trif
luoroethane (R123) and 1-chloro-1,2,2,2-tetrafluoroethane (R124) were measu
red with an adiabatic calorimeter. Temperatures ranged from 167 K for R123
and from 94 K for R124 to 341 K, and pressures were up to 33 MPa. Measureme
nts were conducted an the liquid in equilibrium with its vapor and on compr
essed liquid samples. The samples were of a high purity, verified by chemic
al analysis of each fluid. For the samples, calorimetric results were obtai
ned for two-phase (C-v((2))), saturated liquid (C sigma or C-x'), and singl
e-phase (C-v) molar heat capacities, The C-sigma data were used to estimate
vapor pressures for values less than 100 kPa by applying a thermodynamic r
elationship between the saturated liquid heat capacity and the temperature
derivatives of the vapor pressure. Doe ro the tendency of both R123 and R12
4 to subcool, the triple-point temperature (T-tr) and the enthalpy of fusio
n (Delta H-fus) could not be measured. The principal sources of uncertainty
al e the temperature rise measurement and the change-of-volume work adjust
ment. The expanded uncertainty (at the 2 sigma level) for C-v is estimated
to be 0.7%, for C-v((2)) it is 0.5%, and for C-sigma it is 0.7%.