Subatmospheric vapor pressures for fluoromethane (R41), 1,1-difluoroethane(R152a), and 1,1,1-trifluoroethane (R143a) evaluated from internal-energy measurements
Ha. Duarte-garza et Jw. Magee, Subatmospheric vapor pressures for fluoromethane (R41), 1,1-difluoroethane(R152a), and 1,1,1-trifluoroethane (R143a) evaluated from internal-energy measurements, INT J THERM, 20(5), 1999, pp. 1467-1481
Vapor pressures were evaluated from measured internal-energy changes Delta
U-(2) in the vapor + liquid two-phase region. The method employed a thermod
ynamic relationship between the derivative quantity (partial derivative U-(
2)/partial derivative V)(T), the vapor pressure p(sigma), and its temperatu
re derivative (partial derivative p/partial derivative T)(sigma). This meth
od was applied at temperatures between the triple point and the normal boil
ing point of three substances: fluoromethane (R41), 1,1-difluoroethane (R15
2a), and 1,1,1-trifluoroethane (R143a). In the case of R41, vapor pressures
up to 1 MPa were calculated to validate the technique at higher pressures.
For R152a, the calculated vapor pressure at the triple-point temperature d
iffered from a direct experimental measurement by less than the claimed unc
ertainty (5 Pa) of the measurement. The calculated vapor pressures for R41
helped to resolve discrepancies in several published vapor pressure sources
. Agreement with experimentally measured vapor pressures for R152a and for
R143a near the normal boiling point (101.325 kPa) was within the experiment
al uncertainty of approximately 0.04 kPa (0.04%) for the published measurem
ents.