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CapMachine/CapMachine.Wpf/PPCalculation/REFPROP/FLUIDS/R365MFC.FLD

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R365mfc !Short name
406-58-6 !CAS number
1,1,1,3,3-Pentafluorobutane !Full name
CF3CH2CF2CH3 !Chemical formula {C4H5F5}
HFC-365mfc !Synonym
148.07452 !Molar mass [g/mol]
239.0 !Triple point temperature [K]
313.343 !Normal boiling point [K]
460.0 !Critical temperature [K]
3266.0 !Critical pressure [kPa]
3.2 !Critical density [mol/L]
0.377 !Acentric factor
3.807 !Dipole moment [Debye]; DIPPR DIADEM 2012
IIR !Default reference state
10.0 !Version number
???? !UN Number :UN:
halocb !Family :Family:
???? !Heating value (upper) [kJ/mol] :Heat:
794. !GWP (IPCC 2007) :GWP:
1S/C4H5F5/c1-3(5,6)2-4(7,8)9/h2H2,1H3 !Standard InChI String :InChi:
WZLFPVPRZGTCKP-UHFFFAOYSA-N !Standard InChI Key :InChiKey:
???? !Alternative fluid for mixing rules :AltID:
9d316cb0 !Hash number from InChI Key :Hash:
!The fluid files contain general information about the fluid in the first 15 to 20 lines, followed by sections for the
! equations of state, transport equations, and auxiliary equations. Equations of state are listed first. The NIST recommended
! equations begin with a hash mark (#). The secondary equations begin with the @ symbol. These symbols can be swapped to
! select a secondary equation as primary and the primary as secondary. The equation of state section also contains auxiliary
! equations for the ideal gas heat capacity or ideal gas Helmholtz energy. Below the equations of state (both primary and
! secondary) are the transport equations, first viscosity and then thermal conductivity. These are then followed by the
! secondary equations if available. The transport section also contains auxiliary equations required to calculate either the
! dilute gas state or the critical enhancement. At the end of the file are additional but not necessary auxiliary equations,
! including simple equations for the vapor pressure, saturated liquid and vapor densities, melting line (for some fluids), and
! sublimation line (for even fewer fluids). This section also contains the equations for dielectric constant and surface
! tension if available. The sections are divided by different symbols (these being _-+=^*~) to aid the eye in locating a
! particular section. Secondary equations are indented 10 spaces to avoid confusion with the NIST recommended equations. The
! end of the fluid file is marked with @END. Anything below that is ignored.
! compiled by E.W. Lemmon, NIST Physical and Chemical Properties Division, Boulder, Colorado
! 04-24-00 EWL, Original version.
! 09-18-01 EWL, Finalize equation.
! 10-23-06 EWL, Add new equation of Lemmon.
! 11-13-06 MLH, Add LJ parameters.
! 02-01-07 EWL, Add finalized equation of state.
! 01-24-08 MLH, Revise transport parameters based on available data.
! 08-17-10 IDC, Add ancillary equations.
! 12-06-12 EWL, Add surface tension coefficients of Mulero et al. (2012).
! 04-06-13 EWL, Add dipole moment.
! 08-04-15 EWL, Minor update to match new manuscript. Refit the saturated density ancillaries.
! 11-16-17 MLH, Revised thermal conductivity, viscosity
________________________________________________________________________________
#EOS !---Equation of state---
FEQ !Helmholtz equation of state for R-365mfc of Lemmon and Span (2015).
:TRUECRITICALPOINT: 460.0 3.2 !True EOS critical point [K, mol/L] (where dP/dD=0 and d^2P/dD^2=0 at constant T)
:DOI: 10.1021/acs.jced.5b00684
?
?```````````````````````````````````````````````````````````````````````````````
?Lemmon, E.W. and Span, R.,
? "Thermodynamic Properties of R-227ea, R-365mfc, R-115, and R-13I1,"
? J. Chem. Eng. Data, 60(12):3745-3758, 2015. doi: 10.1021/acs.jced.5b00684
?
?The uncertainties in densities of the equation of state range from
? 0.1 % in the liquid to 1 % near the critical point, and the uncertainty in the
? speeds of sound is 0.05 %. The uncertainty in heat capacities is 2 %, and the
? uncertainty in vapor pressures is 0.25 % at temperatures between 280 K and 360 K.
? In the critical region, the uncertainties are higher for all properties.
?
!```````````````````````````````````````````````````````````````````````````````
239.0 !Lower temperature limit [K]
500.0 !Upper temperature limit [K]
35000.0 !Upper pressure limit [kPa]
9.3 !Maximum density [mol/L]
CPP !Pointer to Cp0 model
148.07452 !Molar mass [g/mol]
239.0 !Triple point temperature [K]
2.478 !Pressure at triple point [kPa]
9.3 !Density at triple point [mol/L]
313.343 !Normal boiling point temperature [K]
0.377 !Acentric factor
460.0 3266.0 3.2 !Tc [K], pc [kPa], rhoc [mol/L]
460.0 3.2 !Reducing parameters [K, mol/L]
8.3144598 !Gas constant [J/mol-K]
11 4 4 12 0 0 0 0 0 0 0 0 !# terms and # coefs/term for normal terms, Gaussian terms, and Gao terms
0.0665967 1.0 4. 0. !a(i),t(i),d(i),l(i)
2.20027 0.24 1. 0.
-2.86240 0.67 1. 0.
0.384559 0.50 2. 0.
-0.621227 1.25 2. 0.
-1.19383 3.35 1. 1.
0.635935 2.50 3. 1.
0.461728 0.96 6. 1.
-0.533472 1.07 6. 1.
-1.07101 5.60 2. 2.
0.139290 6.90 3. 2.
-0.385506 3.0 1. 2. 2. -0.97 -1.07 1.48 1.02 0. 0. 0.
0.885653 3.60 1. 2. 2. -0.94 -1.08 1.49 0.62 0. 0. 0.
0.226303 5.0 1. 2. 2. -2.15 -10.9 1.01 0.53 0. 0. 0.
-0.166116 1.25 2. 2. 2. -2.66 -22.6 1.16 0.48 0. 0. 0.
eta beta gamma epsilon
EXP[eta*(delta-epsilon)^2+beta*(tau-gamma)^2]
#AUX !---Auxiliary function for Cp0
CPP !Ideal gas heat capacity function for R-365mfc of Lemmon and Span (2015).
?
?```````````````````````````````````````````````````````````````````````````````
?Lemmon, E.W. and Span, R., 2006.
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
1.0 8.3144598 !Reducing parameters for T, Cp0
1 2 0 0 0 0 0 !Nterms: polynomial, exponential, cosh, sinh
4.0 0.0
17.47 569.0
16.29 2232.0
#AUX !---Auxiliary function for PX0
PX0 !Helmholtz energy ideal-gas function for R-365mfc of Lemmon and Span (2015).
?
?```````````````````````````````````````````````````````````````````````````````
?Lemmon, E.W. and Span, R., 2006.
?
!```````````````````````````````````````````````````````````````````````````````
1 2 2 0 0 0 0 0 !Nterms: ai*log(tau**ti); ai*tau**ti; ai*log(1-exp(bi*tau))
3.0 1.0 !ai, ti for [ai*log(tau**ti)] terms
-16.3423753778466221 0.0 !aj, ti for [ai*tau**ti] terms
10.2889732266128267 1.0 !aj, ti for [ai*tau**ti] terms
17.47 569.0 !aj, ti for [ai*log(1-exp(-ti/T)] terms
16.29 2232.0
#AUX !---Auxiliary function for PH0
PH0 !Ideal gas Helmholtz form for R-365mfc.
?
?```````````````````````````````````````````````````````````````````````````````
?Lemmon, E.W. and Span, R., 2006.
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
1 2 2 0 0 0 0 0 !Nterms: ai*log(tau**ti); ai*tau**ti; ai*log(1-exp(bi*tau)); cosh; sinh
3.0 1.0 !ai, ti for [ai*log(tau**ti)] terms
-16.3423704513 0.0 !aj, ti for [ai*tau**ti] terms
10.2889710846 1.0
17.47 -1.2369565217 !aj, ti for [ai*log(1-exp(ti*tau)] terms
16.29 -4.852173913
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
#TRN !---ECS Transport---
ECS !Extended Corresponding States model (R134a reference); fit to limited data for R-365mfc.
:DOI: 10.6028/NIST.IR.8209
?
?```````````````````````````````````````````````````````````````````````````````
?Huber, M.L., "Models for the Viscosity, Thermal Conductivity, and Surface Tension
? of Selected Pure Fluids as Implemented in REFPROP v10.0," NISTIR 8209, 2018.
? doi: 10.6028/NIST.IR.8209
?
?VISCOSITY
? The ECS parameters for viscosity were based on the data of: Froba, A.P., Krzeminski, K, and Leipertz, A., "Thermophysical Properties of 1,1,1,3,3-Pentafluorobutane (R365mfc)," Int. J. Thermophys., 25(4):987-1004, 2004. doi: 10.1023/B:IJOT.0000038495.23799.42
? Average absolute deviations of the fit from the experimental data are:
? Froba: AAD 0.4% (Max 1.3%) for saturated liquid over 253 K to 373 K.
?
?THERMAL CONDUCTIVITY
? The ECS parameters for viscosity were based on the data of:
? Froba, A.P., Krzeminski, K, and Leipertz, A., "Thermophysical Properties of 1,1,1,3,3-Pentafluorobutane (R365mfc)," Int. J. Thermophys., 25(4):987-1004. doi: 10.1023/B:IJOT.0000038495.23799.42
? Marrucho, I.M., Oliveira, N.S., and Dohrn, R., "Vapor-Phase Thermal Conductivity, Vapor Pressure, and Liquid Density of R365mfc," J. Chem. Eng. Data, 47:554-558, 2002.
? Average absolute deviations of the fit from the experimental data are:
? Froba: AAD: 1.8% (max 4.5%) for saturated liquid phase from 263 K to 333 K.
? Marrucho: AAD: 0.4% (max-1.0%) for gas phase 336 K to 377 K at pressures to 0.4 MPa.
?
?The Lennard-Jones parameters were estimated with the method of Chung, T.H., Ajlan, M., Lee, L.L., and Starling, K.E., "Generalized Multiparameter Correlation for Nonpolar and Polar Fluid Transport Properties," Ind. Eng. Chem. Res., 27:671-679, 1988.
?
!```````````````````````````````````````````````````````````````````````````````
239.0 !Lower temperature limit [K]
500.0 !Upper temperature limit [K]
35000.0 !Upper pressure limit [kPa]
9.32 !Maximum density [mol/L]
FEQ R134A.FLD
VS1 !Model for reference fluid viscosity
TC1 !Model for reference fluid thermal conductivity
NUL !Large molecule identifier
1 !Lennard-Jones flag (0 or 1) (0 => use estimates)
0.5490 !Lennard-Jones coefficient sigma [nm]
365.28 !Lennard-Jones coefficient epsilon/kappa [K]
3 0 0 !Number of terms in f_int term in Eucken correlation, spare1, spare2
4.115810e-3 0. 0. 0. !Coefficient, power of T, spare1, spare2
-1.70975e-5 1. 0. 0. !Coefficient, power of T, spare1, spare2
2.55262e-8 2. 0. 0. !Coefficient, power of T, spare1, spare2
3 0 0 !Number of terms in psi (visc shape factor): poly,spare1,spare2
0.670823 0. 0. 0. !Coefficient, power of Tr, power of Dr, spare
0.316208 0. 1. 0. !Coefficient, power of Tr, power of Dr, spare
-6.80077e-2 0. 2. 0. !Coefficient, power of Tr, power of Dr, spare
2 0 0 !Number of terms in chi (t.c. shape factor): poly,spare1,spare2
0.434182 0. 0. 0. !Coefficient, power of Tr, power of Dr, spare
0.229206 0. 1. 0. !Coefficient, power of Tr, power of Dr, spare
TK3 !Pointer to critical enhancement auxiliary function
#AUX !---Auxiliary function for the thermal conductivity critical enhancement
TK3 !Simplified thermal conductivity critical enhancement for R-365mfc of Perkins et al. (2013).
?
?```````````````````````````````````````````````````````````````````````````````
?Perkins, R.A., Sengers, J.V., Abdulagatov, I.M., and Huber, M.L.,
? "Simplified Model for the Critical Thermal-Conductivity Enhancement in Molecular Fluids,"
? Int. J. Thermophys., 34(2):191-212, 2013. doi: 10.1007/s10765-013-1409-z
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
9 0 0 0 !# terms: terms, spare, spare, spare
1.0 1.0 1.0 !Reducing parameters for T, rho, tcx [mW/(m-K)]
0.63 !Nu (universal exponent)
1.239 !Gamma (universal exponent)
1.02 !R0 (universal amplitude)
0.063 !Z (universal exponent--not used for t.c., only viscosity)
1.0 !C (constant in viscosity eqn = 1/[2 - (alpha + gamma)/(2*nu)], but often set to 1)
0.218e-9 !Xi0 (amplitude) [m]
0.060 !Gam0 (amplitude) [-]
0.669e-9 !Qd_inverse (modified effective cutoff parameter) [m]; value used for R134a
690.0 !Tref (reference temperature)
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
#STN !---Surface tension---
ST1 !Surface tension model for R-365mfc of Mulero et al. (2012).
:DOI: 10.1063/1.4768782
?
?```````````````````````````````````````````````````````````````````````````````
?Mulero, A., Cachadiña, I., and Parra, M.I.,
? "Recommended Correlations for the Surface Tension of Common Fluids,"
? J. Phys. Chem. Ref. Data, 41(4), 043105, 2012. doi: 10.1063/1.4768782
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
1 !Number of terms in surface tension model
460 !Critical temperature used in fit (dummy)
0.0534 1.21 !Sigma0 and n
#PS !---Vapor pressure---
PS5 !Vapor pressure equation for R-365mfc of Lemmon and Span (2015).
?
?```````````````````````````````````````````````````````````````````````````````
?Functional Form: P=Pc*EXP[SUM(Ni*Theta^ti)*Tc/T] where Theta=1-T/Tc, Tc and Pc
? are the reducing parameters below, which are followed by rows containing Ni and ti.
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
460.0 3266.0 !Reducing parameters
5 0 0 0 0 0 !Number of terms in equation
-8.0955 1.0
2.0414 1.5
-13.333 3.4
25.514 4.3
-19.967 5.0
#DL !---Saturated liquid density---
DL1 !Saturated liquid density equation for R-365mfc of Lemmon and Span (2015).
?
?```````````````````````````````````````````````````````````````````````````````
?Functional Form: D=Dc*[1+SUM(Ni*Theta^ti)] where Theta=1-T/Tc, Tc and Dc are
? the reducing parameters below, which are followed by rows containing Ni and ti.
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
460.0 3.2 !Reducing parameters
5 0 0 0 0 0 !Number of terms in equation
1.7667 0.31
-1.6156 0.6
8.1107 0.9
-10.439 1.2
5.0346 1.5
#DV !---Saturated vapor density---
DV3 !Saturated vapor density equation for R-365mfc of Lemmon and Span (2015).
?
?```````````````````````````````````````````````````````````````````````````````
?Functional Form: D=Dc*EXP[SUM(Ni*Theta^ti)] where Theta=1-T/Tc, Tc and Dc are
? the reducing parameters below, which are followed by rows containing Ni and ti.
?
!```````````````````````````````````````````````````````````````````````````````
0. !
10000. !
0. !
0. !
460.0 3.2 !Reducing parameters
4 0 0 0 0 0 !Number of terms in equation
-1.4964 0.271
-6.5917 0.88
-21.364 2.85
-70.331 6.7
@END
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