📄 r123.fld
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R123 !short name
306-83-2 !CAS number
2,2-dichloro-1,1,1-trifluoroethane !full name
CHCl2CF3 !chemical formula
HCFC-123 !synonym
152.931 !molecular weight [g/mol]
166.0 !triple point temperature [K]
300.973 !normal boiling point [K]
456.831 !critical temperature [K]
3661.8 !critical pressure [kPa]
3.596417 !critical density [mol/L]
0.28192 !acentric factor
1.356 !dipole moment [Debye]; Meyer & Morrison (1991) J. Chem. Eng. Data 36:409-413.
IIR !default reference state
6.1 !version number
! compiled by M. McLinden, NIST Physical and Chemical Properties Division, Boulder, Colorado
! 10-10-95 MM, original version
! 03-15-96 MM, add transport correlations compiled by S.A. Klein
! 03-18-96 MM, add dipole moment
! 06-17-96 MM, add thermal conductivity coefficients fitted by S.A. Klein
! 08-19-96 MM, add surface tension fit
! 01-31-97 MM, change pointer for ECS reference viscosity from VS3 to VS1
! put viscosity model of Tanaka and Sotani into new VS1 form
! 02-20-97 MM, add default reference state
! 02-25-97 MM, add thermal conductivity correlation of Laesecke
! 02-26-97 MM, add version number and pointer to visc critical enhancement (both future use)
! 03-11-97 MM, modify ECS-transport to new format
! 03-25-97 MM, set Psi,Chi coeff in ECS-transport to 1,0 pending refit of data
! 08-21-97 MM, purge exponentials from values read by GUI (e.g. model limits)
! 10-24-97 MM, read in f_int term in Eucken correlation in ECS method for t.c.
! change reference fluid EOS for ECS-transport from BWR to FEQ
! 11-01-99 EWL, add Span 12 term short equation of state
! 11-10-99 EWL, change ptp to match p at 166 K
! 01-24-00 EWL, change transport limits to match eos
#EOS !equation of state specification
BWR MBWR equation of state for R-123 of Younglove and McLinden (1994).
?LITERATURE REFERENCE \
?Younglove, B.A. and McLinden, M.O.,
? "An international standard equation-of-state formulation of the thermodynamic
? properties of refrigerant 123 (2,2-dichloro-1,1,1-trifluoroethane),"
? J. Phys. Chem. Ref. Data, 23:731-779, 1994.
?\
?The uncertainties of the equation of state are 0.1% in density, 1.5% in heat
?capacity, and 2% in the speed of sound, except in the critical region.
?The uncertainty in vapor pressure is 0.1%. Uncertainties are greater below
?180 K.
?\
?ABSTRACT \
?A modified Benedict-Webb-Rubin (MBWR) equation of state has been developed
? for Refrigerant 123 (2,2-dichloro-1,1,1-trifluoroethane) based on recently
? measured thermodynamic property data and data available from the literature.
? Single-phase pressure-volume-temperature (PVT), heat capacity, and sound speed
? data, as well as second virial, vapor pressure, and saturated liquid and
? saturated vapor density data, were used with multiproperty linear least
? squares fitting techniques to fit the 32 adjustable coefficients of the MBWR
? equation. Coefficients for the equation of state and for ancillary equations
? representing the vapor pressure, saturated liquid and saturated vapor
? densities, and ideal gas heat capacity are given. While the measurements
? cover differing ranges of temperature and pressure, the MBWR formulation is
? applicable along the saturation line and in the liquid, vapor, and
? supercritical regions at temperatures from 166 to 500 K with pressures to
? 40 MPa and densities to 11.6 mol/L (1774 kg/m3). This formulation has been
? selected as an international standard based on an evaluation of the available
? equations of state by a group working under the auspices of the International
? Energy Agency.
?
!end of info section
166.0 !lower temperature limit [K]
600.0 !upper temperature limit [K]
40000.0 !upper pressure limit [kPa]
11.60 !maximum density [mol/L]
CPP !pointer to Cp0 model
152.931 !molecular weight [g/mol]
166.0 !triple point temperature [K]
0.0042 !pressure at triple point [kPa]
11.60 !density at triple point [mol/L]
300.973 !normal boiling point temperature [K]
0.28192 !acentric factor
456.831 3661.8 3.596417 !Tc [K], pc [kPa], rhoc [mol/L]
456.831 3.596417 !reducing parameters [K, mol/L]
3.596417 !gamma
0.08314510 !gas constant [L-bar/mol-K]
32 1 !Nterm, Ncoeff per term
-0.657453133659d-02 0.293479845842d+01 -0.989140469845d+02
0.201029776013d+05 -0.383566527886d+07 0.227587641969d-02
-0.908726819450d+01 0.434181417995d+04 0.354116464954d+07
-0.635394849670d-03 0.320786715274d+01 -0.131276484299d+04
-0.116360713718d+00 -0.113354409016d+02 -0.537543457327d+04
0.258112416120d+01 -0.106148632128d+00 0.500026133667d+02
-0.204326706346d+01 -0.249438345685d+07 -0.463962781113d+09
-0.284903429588d+06 0.974392239902d+10 -0.637314379308d+04
0.314121189813d+06 -0.145747968225d+03 -0.843830261449d+07
-0.241138441593d+01 0.108508031257d+04 -0.106653193965d-01
-0.121343571084d+02 -0.257510383240d+03
@EOS !equation of state specification
FE1 Helmholtz transform of MBWR EOS for R-123 of Younglove & McLinden (1994)
?LITERATURE REFERENCE \
?Younglove, B.A. and McLinden, M.O.,
? "An international standard equation-of-state formulation of the thermodynamic
? properties of refrigerant 123 (2,2-dichloro-1,1,1-trifluoroethane),"
? J. Phys. Chem. Ref. Data, 23:731-779, 1994.
?\
?The equation here is the same as the Younglove and McLinden BWR equation,
? but has been transformed into the fundamental Helmholtz energy form.
?
!end of info section
166.0 !lower temperature limit [K]
600.0 !upper temperature limit [K]
40000.0 !upper pressure limit [kPa]
11.60 !maximum density [mol/L]
CPP !pointer to Cp0 model
152.931 !molecular weight [g/mol]
166.0 !triple point temperature [K]
0.0042 !pressure at triple point [kPa]
11.60 !density at triple point [mol/L]
300.973 !normal boiling point temperature [K]
0.28192 !acentric factor
456.831 3661.8 3.596417 !Tc [K], pc [kPa], rhoc [mol/L]
456.831 3.596417 !reducing parameters [K, mol/L]
8.314510 !gas constant [J/mol-K]
40 4 0 0 0 0 !# terms, # coeff/term for: "normal" terms, critical, spare
-0.100242647494E+02 3.000 0.00 0 !a(i),t(i),d(i),l(i)
-0.280607656419E+00 4.000 0.00 0
0.206814471606E-01 5.000 0.00 0
-0.284379431451E+00 0.000 1.00 0
0.593928110321E+01 0.500 1.00 0
-0.936560389528E+01 1.000 1.00 0
0.416660793675E+01 2.000 1.00 0
-0.174023292951E+01 3.000 1.00 0
0.177019905365E+00 0.000 2.00 0
-0.154721692260E+01 1.000 2.00 0
0.161820495590E+01 2.000 2.00 0
0.288903529383E+01 3.000 2.00 0
-0.118493874757E+00 0.000 3.00 0
0.130952266209E+01 1.000 3.00 0
-0.117308103711E+01 2.000 3.00 0
-0.128125131950E+00 1.000 4.00 0
-0.786087387513E-01 2.000 5.00 0
-0.816000499305E-01 3.000 5.00 0
0.536451054311E-01 2.000 6.00 0
-0.680078211929E-02 2.000 7.00 0
0.701264082191E-02 3.000 7.00 0
-0.901762397311E-03 3.000 8.00 0
0.100242647494E+02 3.000 0.00 2
0.280607656419E+00 4.000 0.00 2
-0.206814471606E-01 5.000 0.00 2
0.798923878145E+01 3.000 2.00 2
-0.547972072476E+00 4.000 2.00 2
-0.206814470584E-01 5.000 2.00 2
0.249142724365E+01 3.000 4.00 2
-0.273986034884E+00 4.000 4.00 2
0.236001863614E+00 5.000 4.00 2
0.540528251211E+00 3.000 6.00 2
-0.600457561959E-01 4.000 6.00 2
0.786672874826E-01 5.000 6.00 2
0.708085874508E-01 3.000 8.00 2
-0.150114389748E-01 4.000 8.00 2
0.182205199477E-02 5.000 8.00 2
0.314978575163E-02 3.000 10.00 2
0.784455573794E-02 4.000 10.00 2
0.364410397155E-03 5.000 10.00 2
#AUX !auxiliary model specification
CPP ideal gas heat capacity function of Younglove & McLinden (1994).
?LITERATURE REFERENCE \
?Younglove, B.A. and McLinden, M.O.,
? "An international standard equation-of-state formulation of the thermodynamic
? properties of refrigerant 123 (2,2-dichloro-1,1,1-trifluoroethane),"
? J. Phys. Chem. Ref. Data, 23:731-779, 1994.
?\
!end of info section
150.0 !lower temperature limit [K]
500.0 !upper temperature limit [K]
0.0 !upper pressure limit [kPa]
0.0 !maximum density [mol/L]
1.0 1.0 !reducing parameters for T, Cp0
4 0 0 0 0 0 0 !Nterms: polynomial, exponential, cosh, sinh
17.01154d0 0.00 !c(i), power of T
0.4046308d0 1.00
-4.644803d-4 2.00
2.347418d-7 3.00
@EOS !equation of state specification
FES short Helmholtz equation of state for R-123 of Span (2000).
?LITERATURE REFERENCE \
?Span, R.,
? "Multiparameter Equations of State - An Accurate Source of Thermodynamic
? Property Data," Springer, Berlin, Heidelberg, New York, 2000.
?\
?The uncertainties of the equation of state are approximately 0.2% (to
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