一些优化:CAN和PLC地址的优化
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CapMachine.Wpf/PPCalculation/REFPROP/FLUIDS/HYDROGEN.FLD
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CapMachine.Wpf/PPCalculation/REFPROP/FLUIDS/HYDROGEN.FLD
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Hydrogen (normal) !Short name
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1333-74-0 !CAS number
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Hydrogen (normal) !Full name
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H2 !Chemical formula {H2}
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R-702 !Synonym
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2.01588 !Molar mass [g/mol]
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13.957 !Triple point temperature [K]
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20.369 !Normal boiling point [K]
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33.145 !Critical temperature [K]
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1296.4 !Critical pressure [kPa]
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15.508 !Critical density [mol/L]
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-0.219 !Acentric factor
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0.0 !Dipole moment [Debye]; (exactly zero due to symmetry)
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NBP !Default reference state
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10.0 !Version number
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1049 !UN Number :UN:
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cryogen !Family :Family:
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285.83 !Heating value (upper) [kJ/mol] :Heat:
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A3 !Safety Group (ASHRAE Standard 34, 2010) :Safety:
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1S/H2/h1H !Standard InChI String :InChi:
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UFHFLCQGNIYNRP-UHFFFAOYSA-N !Standard InChI Key :InChiKey:
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???? !Alternative fluid for mixing rules :AltID:
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8d757b40 !Hash number from InChI Key :Hash:
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!Quantum mechanics requires orthohydrogen to retain rotational energy at low temperatures, even below the triple point
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! temperature, that manifests in significantly higher ideal-gas thermal properties relative to parahydrogen. The
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! traditional reference state determination method of setting the enthalpy and entropy of an ideal-gas equal to zero for a
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! saturated liquid at the normal boiling point does not account for this difference and results in false comparisons
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! between parahydrogen and orthohydrogen. To allow the orthohydrogen and parahydrogen equations of state to accurately
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! reflect these differences, the reference state properties for orthohydrogen have been set in agreement with those
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! tabulated in LeRoy et al., J. Phys. Chem., 94:923-929, 1990.
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!
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!Here, the reference state for normal hydrogen was left as NBP to conform with that from earlier versions of Refprop.
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! If you wish to obtain enthalpy and entropy properties that are consistent with those now used in the orthohydrogen
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! fluid file, delete line 14 above that has NBP on it and replace it with the following two lines:
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!OT0 !Default reference state that agrees with those of LeRoy et al., J. Phys. Chem., 94:923-929, 1990.
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!25.0 0.1 533.5 124.14244
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!
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!Then open the parahyd.fld file and follow the directions there.
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!The fluid files contain general information about the fluid in the first 15 to 20 lines, followed by sections for the
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! equations of state, transport equations, and auxiliary equations. Equations of state are listed first. The NIST recommended
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! equations begin with a hash mark (#). The secondary equations begin with the @ symbol. These symbols can be swapped to
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! select a secondary equation as primary and the primary as secondary. The equation of state section also contains auxiliary
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! equations for the ideal gas heat capacity or ideal gas Helmholtz energy. Below the equations of state (both primary and
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! secondary) are the transport equations, first viscosity and then thermal conductivity. These are then followed by the
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! secondary equations if available. The transport section also contains auxiliary equations required to calculate either the
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! dilute gas state or the critical enhancement. At the end of the file are additional but not necessary auxiliary equations,
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! including simple equations for the vapor pressure, saturated liquid and vapor densities, melting line (for some fluids), and
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! sublimation line (for even fewer fluids). This section also contains the equations for dielectric constant and surface
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! tension if available. The sections are divided by different symbols (these being _-+=^*~) to aid the eye in locating a
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! particular section. Secondary equations are indented 10 spaces to avoid confusion with the NIST recommended equations. The
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! end of the fluid file is marked with @END. Anything below that is ignored.
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! compiled by E.W. Lemmon, NIST Physical and Chemical Properties Division, Boulder, Colorado
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! 04-02-98 EWL, Original version.
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! 10-20-99 EWL, Add tcx and eta formulations from NIST12, Version 3.1.
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! 11-06-00 EWL, Switch transport equations to hardcoded models.
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! 01-29-02 EWL, Add sublimation line.
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! 07-07-04 EWL, Add Bender EOS.
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! 08-05-04 EWL, Add Harvey and Lemmon dielectric correlation.
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! 11-18-04 MLH, Add tPr coeff.
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! 01-18-05 EWL, Add Kunz and Wagner EOS.
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! 03-27-07 JWL, Add equation of state of Leachman et al. (2009).
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! 10-03-07 EWL, Change upper density limit of vis and tcx from 38 to 43 mol/l; above 43 mol/l, the viscosity equation goes bad.
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! 10-16-07 EWL, Change upper temp. limit of vis and tcx from 400 to 1000 K based on good graphical extrapolation.
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! 07-17-08 EWL, Change incorrect molecular weight from 2.01594 to 2.01588.
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! 07-21-08 EWL, Add vapor pressure ancillary.
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! 06-17-10 CKL, Add ancillary equations for sat. densities.
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! 04-07-11 MLH, Add thermal conductivity model of Assael et al. (2011).
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! 04-07-11 MLH, Add viscosity model of Quinones-Cisneros et al. (2011) but not set as default.
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! 11-15-12 MLH, Add SR viscosity model as default.
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! 12-06-12 EWL, Add surface tension coefficients of Mulero et al. (2012).
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! 05-15-17 EWL, Change the hard coded VS0 model to the VS7 reverse Polish notation.
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________________________________________________________________________________
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#EOS !---Equation of state---
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FEQ !Helmholtz equation of state for normal hydrogen of Leachman et al. (2009).
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:TRUECRITICALPOINT: 33.145 15.508 !True EOS critical point [K, mol/L] (where dP/dD=0 and d^2P/dD^2=0 at constant T)
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:DOI: 10.1063/1.3160306
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Leachman, J.W., Jacobsen, R.T, Penoncello, S.G., and Lemmon, E.W.,
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? "Fundamental Equations of State for Parahydrogen, Normal Hydrogen, and Orthohydrogen,"
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? J. Phys. Chem. Ref. Data, 38(3):721-748, 2009.
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?
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?The uncertainty in density is 0.1% at temperatures from the triple point
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? to 250 K and at pressures up to 40 MPa, except in the critical region,
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? where an uncertainty of 0.2% in pressure is generally attained. In the
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? region between 250 and 450 K and at pressures to 300 MPa, the
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? uncertainty in density is 0.04%. At temperatures between 450 and 1000
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? K, the uncertainty in density increases to 1%. At pressures between 300
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? and 2000 MPa, the uncertainty in density is 8%. Speed of sound data are
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? represented within 0.5% below 100 MPa. The estimated uncertainty for
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? heat capacities is 1.0%. The estimated uncertainties of vapor pressures
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? and saturated liquid densities calculated with the Maxwell criterion
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? are 0.2% for each property.
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?
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!```````````````````````````````````````````````````````````````````````````````
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13.957 !Lower temperature limit [K]
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1000.0 !Upper temperature limit [K]
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2000000.0 !Upper pressure limit [kPa]
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102.0 !Maximum density [mol/L]
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CPP !Pointer to Cp0 model
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2.01588 !Molar mass [g/mol]
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13.957 !Triple point temperature [K]
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7.3578 !Pressure at triple point [kPa]
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38.2 !Density at triple point [mol/L]
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20.369 !Normal boiling point temperature [K]
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-0.219 !Acentric factor
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33.145 1296.4 15.508 !Tc [K], pc [kPa], rhoc [mol/L]
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33.145 15.508 !Reducing parameters [K, mol/L]
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8.314472 !Gas constant [J/mol-K]
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9 4 5 12 0 0 0 0 0 0 0 0 !# terms and # coefs/term for normal terms, Gaussian terms, and Gao terms
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0.01 1.0 4. 0. !a(i),t(i),d(i),l(i)
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-6.93643 0.6844 1. 0.
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2.1101 0.989 1. 0.
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4.52059 0.489 1. 0.
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0.732564 0.803 2. 0.
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-1.34086 1.1444 2. 0.
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0.130985 1.409 3. 0.
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-0.777414 1.754 1. 1.
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0.351944 1.311 3. 1.
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-0.0211716 4.187 2. 2. 2. -1.685 -0.171 0.7164 1.506 0. 0. 0.
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0.0226312 5.646 1. 2. 2. -0.489 -0.2245 1.3444 0.156 0. 0. 0.
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0.032187 0.791 3. 2. 2. -0.103 -0.1304 1.4517 1.736 0. 0. 0.
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-0.0231752 7.249 1. 2. 2. -2.506 -0.2785 0.7204 0.67 0. 0. 0.
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0.0557346 2.986 1. 2. 2. -1.607 -0.3967 1.5445 1.662 0. 0. 0.
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eta beta gamma epsilon
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EXP[eta*(delta-epsilon)^2+beta*(tau-gamma)^2]
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#AUX !---Auxiliary function for Cp0
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CPP !Ideal gas heat capacity function for normal hydrogen of Leachman et al. (2009).
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Leachman, J.W., Jacobsen, R.T, Penoncello, S.G., and Lemmon, E.W., 2009.
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?
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!```````````````````````````````````````````````````````````````````````````````
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0. !
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10000. !
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0. !
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0. !
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1.0 8.314472 !Reducing parameters for T, Cp0
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1 5 0 0 0 0 0 !Nterms: polynomial, exponential, cosh, sinh
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2.5 0.0
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1.616 531.0
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-0.4117 751.0
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-0.792 1989.0
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0.758 2484.0
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1.217 6859.0
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#AUX !---Auxiliary function for PX0
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PX0 !Helmholtz energy ideal-gas function for normal hydrogen of Leachman et al. (2009).
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Leachman, J.W., Jacobsen, R.T, Penoncello, S.G., and Lemmon, E.W., 2009.
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?
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!```````````````````````````````````````````````````````````````````````````````
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1 2 5 0 0 0 0 0 !Nterms: ai*log(tau**ti); ai*tau**ti; ai*log(1-exp(bi*tau))
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1.5 1.0 !ai, ti for [ai*log(tau**ti)] terms
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-1.4579850777108838 0.0 !aj, ti for [ai*tau**ti] terms
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1.8880764164897215 1.0 !aj, ti for [ai*tau**ti] terms
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1.616 531.0 !aj, ti for [ai*log(1-exp(-ti/T)] terms
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-0.4117 751.0
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-0.792 1989.0
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0.758 2484.0
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1.217 6859.0
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#AUX !---Auxiliary function for PH0
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PH0 !Ideal gas Helmholtz form for hydrogen (normal).
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Leachman, J.W., Jacobsen, R.T, Penoncello, S.G., and Lemmon, E.W., 2009.
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?
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!```````````````````````````````````````````````````````````````````````````````
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0. !
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10000. !
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0. !
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0. !
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1 2 5 0 0 0 0 0 !Nterms: ai*log(tau**ti); ai*tau**ti; ai*log(1-exp(bi*tau)); cosh; sinh
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1.5 1.0 !ai, ti for [ai*log(tau**ti)] terms
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-1.4579856475 0.0 !aj, ti for [ai*tau**ti] terms
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1.888076782 1.0
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1.616 -16.0205159149 !aj, ti for [ai*log(1-exp(ti*tau)] terms
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-0.4117 -22.6580178006
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-0.792 -60.0090511389
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0.758 -74.9434303817
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1.217 -206.9392065168
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--------------------------------------------------------------------------------
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@EOS !---Equation of state---
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FEK !Helmholtz equation of state for hydrogen of Kunz and Wagner (2004).
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Kunz, O., Klimeck, R., Wagner, W., Jaeschke, M.
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? "The GERG-2004 Wide-Range Equation of State for Natural Gases
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? and Other Mixtures," GERG Technical Monograph 15,
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? Fortschritt-Berichte VDI, VDI-Verlag, Düsseldorf, 2007.
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?
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!```````````````````````````````````````````````````````````````````````````````
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13.957 !Lower temperature limit [K]
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400.0 !Upper temperature limit [K]
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121000.0 !Upper pressure limit [kPa]
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38.148 !Maximum density [mol/L]
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PHK !Pointer to Cp0 model
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2.01588 !Molar mass [g/mol]
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13.957 !Triple point temperature [K]
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6.669 !Pressure at triple point [kPa]
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38.33 !Density at triple point [mol/L]
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20.38 !Normal boiling point temperature [K]
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-0.2187 !Acentric factor
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33.19 1315.0 14.94 !Tc [K], pc [kPa], rhoc [mol/L]
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33.19 14.94 !Reducing parameters [K, mol/L]
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8.314472 !Gas constant [J/mol-K]
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14 4 0 0 0 0 0 0 0 0 0 0 !# terms and # coefs/term for normal terms, Gaussian terms, and Gao terms
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5.3579928451252 0.5 1. 0.
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-6.2050252530595 0.625 1. 0.
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0.13830241327086 0.375 2. 0.
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-0.071397954896129 0.625 2. 0.
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0.015474053959733 1.125 4. 0.
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-0.14976806405771 2.625 1. 1.
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-0.026368723988451 0.0 5. 1.
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0.056681303156066 0.25 5. 1.
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-0.060063958030436 1.375 5. 1.
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-0.45043942027132 4.0 1. 2.
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0.424788402445 4.25 1. 2.
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-0.021997640827139 5.0 2. 3.
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-0.01049952137453 8.0 5. 3.
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-0.0028955902866816 8.0 1. 5.
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@AUX !---Auxiliary function for PH0
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PHK !Ideal gas Helmholtz form for hydrogen of Kunz and Wagner (2004).
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?
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?```````````````````````````````````````````````````````````````````````````````
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?Kunz, O., Klimeck, R., Wagner, W., Jaeschke, M.
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? "The GERG-2004 Wide-Range Equation of State for Natural Gases
|
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? and Other Mixtures," GERG Technical Monograph 15,
|
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? Fortschritt-Berichte VDI, VDI-Verlag, Düsseldorf, 2007.
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?
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!```````````````````````````````````````````````````````````````````````````````
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0. !
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10000. !
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0. !
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0. !
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1 2 0 2 2 0 0 0 !Nterms: ai*log(tau**ti); ai*tau**ti; ai*log(1-exp(bi*tau)); cosh; sinh
|
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1.47906 1.0 !ai, ti for [ai*log(tau**ti)] terms
|
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13.796443393 0.0 !aj, ti for [ai*tau**ti] terms
|
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-175.864487294 1.0
|
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-0.45444 9.84763483 !aj, ti for cosh and sinh terms
|
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1.3756 50.367279301
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0.95806 6.891654113
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1.56039 49.76529075
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@EOS !---Equation of state---
|
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FE1 !Helmholtz equation of state for hydrogen of Bender (1982).
|
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?
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?```````````````````````````````````````````````````````````````````````````````
|
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?Bender, E.
|
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? "Equation of state of normal hydrogen in the range 18 to 700 K and 1 to 500 bar,"
|
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? VDI Forschungsheft N 609, pp. 15-20, 1982.
|
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?
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?Cp0 equation was taken from McCarty et al. (1981) since Bender equation is
|
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? split in two pieces from 10 to 250 K and from 250 to 600 K.
|
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?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
18.0 !Lower temperature limit [K]
|
||||
700.0 !Upper temperature limit [K]
|
||||
50000.0 !Upper pressure limit [kPa]
|
||||
38.74 !Maximum density [mol/L] (change to 41 when melting line is added)
|
||||
CP1 !Pointer to Cp0 model
|
||||
2.01594 !Molar mass [g/mol]
|
||||
13.957 !Triple point temperature [K]
|
||||
8.736 !Pressure at triple point [kPa]
|
||||
38.7 !Density at triple point [mol/L]
|
||||
20.39 !Normal boiling point temperature [K]
|
||||
-0.218 !Acentric factor
|
||||
33.24 1303.0 15.37744 !Tc [K], pc [kPa], rhoc [mol/L]
|
||||
33.24 15.37744 !Reducing parameters [K, mol/L]
|
||||
8.3143 !Gas constant [J/mol-K]
|
||||
22 5 0 0 0 0 0 0 0 0 0 0 !# terms and # coefs/term for normal terms, Gaussian terms, and Gao terms
|
||||
1.33442326203 3. 0. 0. 0. !a(i),t(i),d(i),l(i)
|
||||
-1.04116843433 4. 0. 0. 0.
|
||||
0.227202245707 5. 0. 0. 0.
|
||||
0.300374270906 0. 1. 0. 0.
|
||||
-0.463984214813 1. 1. 0. 0.
|
||||
-1.78010492282 2. 1. 0. 0.
|
||||
1.00460103605 3. 1. 0. 0.
|
||||
-0.187200622541 4. 1. 0. 0.
|
||||
0.00980276957749 0. 2. 0. 0.
|
||||
0.0543224866339 1. 2. 0. 0.
|
||||
-0.026349631261 2. 2. 0. 0.
|
||||
0.0315432315759 0. 3. 0. 0.
|
||||
-0.0525788294155 1. 3. 0. 0.
|
||||
-0.00685380627808 0. 4. 0. 0.
|
||||
0.0344540276656 1. 4. 0. 0.
|
||||
-0.000555747275982 1. 5. 0. 0.
|
||||
-1.33442326203 3. 0. 2. 0.711139834571
|
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1.04116843433 4. 0. 2. 0.711139834571
|
||||
-0.227202245707 5. 0. 2. 0.711139834571
|
||||
-0.378598758038 3. 2. 2. 0.711139834571
|
||||
0.249888797892 4. 2. 2. 0.711139834571
|
||||
-0.0498847982876 5. 2. 2. 0.711139834571
|
||||
|
||||
|
||||
@EOS !---Equation of state---
|
||||
BWR !MBWR equation of state for hydrogen of Younglove (1982).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Younglove, B.A.,
|
||||
? "Thermophysical Properties of Fluids. I. Argon, Ethylene,
|
||||
? Parahydrogen, Nitrogen, Nitrogen Trifluoride, and Oxygen,"
|
||||
? J. Phys. Chem. Ref. Data, Vol. 11, Suppl. 1, pp. 1-11, 1982.
|
||||
?
|
||||
?The uncertainties in density are 0.1% in the liquid phase, 0.25% in the
|
||||
? vapor phase, and 0.2% in the supercritical region. The uncertainty in
|
||||
? heat capacity is 3% and the uncertainty in speed of sound is 2% in the
|
||||
? liquid phase and 1% elsewhere.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
400.0 !Upper temperature limit [K]
|
||||
121000.0 !Upper pressure limit [kPa]
|
||||
38.148 !Maximum density [mol/L]
|
||||
CP1 !Pointer to Cp0 model
|
||||
2.01594 !Molar mass [g/mol]
|
||||
13.957 !Triple point temperature [K]
|
||||
7.70 !Pressure at triple point [kPa]
|
||||
38.3 !Density at triple point [mol/L]
|
||||
20.39 !Normal boiling point temperature [K]
|
||||
-0.214 !Acentric factor
|
||||
33.19 1315.0 14.94 !Tc [K], pc [kPa], rhoc [mol/L]
|
||||
33.19 14.94 !Reducing parameters [K, mol/L]
|
||||
15.6173762 !gamma
|
||||
0.0831434 !Gas constant [L-bar/mol-K]
|
||||
32 1 !Nterm, Ncoeff per term
|
||||
0.0004675528393416 0.04289274251454 -0.5164085596504
|
||||
2.961790279801 -30.27194968412 0.1908100320379e-4
|
||||
-0.001339776859288 0.3056473115421 51.61197159532
|
||||
0.1999981550224e-6 0.0002896367059356 -0.02257803939041
|
||||
-0.2287392761826e-5 0.2446261478645e-4 -0.001718181601119
|
||||
-0.5465142603459e-6 0.4051941401315e-8 0.1157595123961e-5
|
||||
-0.1269162728389e-7 -49.83023605519 -160.6676092098
|
||||
-0.192679918531 9.319894638928 -0.0003222596554434
|
||||
0.001206839307669 -0.384158819747e-6 -0.4036157453608e-4
|
||||
-0.1250868123513e-9 0.1976107321888e-8 -0.2411883474011e-12
|
||||
-0.4127551498251e-12 0.891797288361e-11
|
||||
|
||||
|
||||
@AUX !---Auxiliary function for Cp0
|
||||
CP1 !Ideal gas heat capacity function for hydrogen (normal).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?McCarty, R.D., Hord, J., and Roder, H.M.,
|
||||
? "Selected Properties of Hydrogen (Engineering Design Data),"
|
||||
? NBS Monograph 168, National Bureau of Standards, Boulder, 1981.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
0. !
|
||||
10000. !
|
||||
0. !
|
||||
0. !
|
||||
1.0 8.31434 !Reducing parameters for T, Cp0
|
||||
17 0 0 0 0 0 0 !Nterms: polynomial, exponential, cosh, sinh
|
||||
0.12155215e+11 -7.0
|
||||
-0.36396763e+10 -6.0
|
||||
433752650.0 -5.0
|
||||
-23085817.0 -4.0
|
||||
-3868.0927 -3.0
|
||||
88240.136 -2.0
|
||||
-7858.7085 -1.0
|
||||
724.80209 0.0
|
||||
-184.26806 0.5
|
||||
21.80155 1.0
|
||||
-1.305182 1.5
|
||||
0.021003175 2.0
|
||||
0.0023911604 2.5
|
||||
-0.00018240547 3.0
|
||||
0.0000056149561 3.5
|
||||
-0.7380331e-7 4.0
|
||||
0.66357755e-11 5.0
|
||||
|
||||
|
||||
@EOS !---Cubic equation of state---
|
||||
PRT !Translated Peng-Robinson equation for hydrogen (normal).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Volume translation of Peng Robinson EOS.
|
||||
? Translation computed so that sat. liquid density at T=27K matches MBWR equation
|
||||
? of state for H2 of Younglove (1982).
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
400.0 !Upper temperature limit [K]
|
||||
121000.0 !Upper pressure limit [kPa]
|
||||
38.148 !Maximum density [mol/L]
|
||||
CPP !Pointer to Cp0 model
|
||||
2.01594 !Molar mass [g/mol]
|
||||
-0.214 !Acentric factor
|
||||
33.19 !Critical temperature [K]
|
||||
1315.0 !Critical pressure [kPa]
|
||||
14.94 !Critical density [mol/L]
|
||||
8.314472 !Gas constant [J/mol-K]
|
||||
1 !Number of parameters
|
||||
-0.004803
|
||||
|
||||
|
||||
|
||||
|
||||
^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
|
||||
|
||||
#ETA !---Viscosity---
|
||||
VS7 !Pure fluid viscosity model from symbolic regression for hydrogen (normal) of Muzny et al. (2013).
|
||||
:DOI: 10.1021/je301273j
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Muzny, C.D., Huber, M.L., and Kazakov, A.F.,
|
||||
? "Correlation for the Viscosity of Normal Hydrogen Obtained from Symbolic Regression,"
|
||||
? J. Chem. Eng. Data, 58:969-979, 2013.
|
||||
?
|
||||
?The estimated uncertainty is 4% for the saturated liquid from the triple point
|
||||
? to 31 K, with larger deviations as the critical region is approached. The
|
||||
? estimated uncertainty is 4% for the supercritical fluid phase at pressures
|
||||
? to 200 MPa. For the limited range of 200 K to 400 K at pressures up to
|
||||
? 0.1 MPa, the uncertainty is 0.1%.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
2000.0 !Upper temperature limit [K]
|
||||
2000000.0 !Upper pressure limit [kPa]
|
||||
102.0 !Maximum density [mol/L]
|
||||
NUL !Pointer to collision integral model
|
||||
!
|
||||
!Dilute gas function
|
||||
$DG RED SUMLOGT:5 EXP CNST SQR * INV SUM:1 CNST * SQRT *
|
||||
!
|
||||
!Second viscosity virial function
|
||||
$VV RED SUM:7 CNST CUBE *
|
||||
!
|
||||
!Residual function
|
||||
$RF RED SUM:3 SUM:1 SUM:2 / + EXP SUM:1 *
|
||||
!
|
||||
!Coefficients
|
||||
$CF
|
||||
0.021357 30.41 1. 0. 0 !Reducing parameters for eta, T, rho
|
||||
0.209630 0. 0. 0. 0 ! s1*LOG(Ts) Coefficient to match Moldover
|
||||
-0.455274 1. 0. 0. 0 ! s2*LOG(Ts)
|
||||
0.143602 2. 0. 0. 0 ! s3*LOG(Ts)^2
|
||||
-0.0335325 3. 0. 0. 0 ! s4*LOG(Ts)^3
|
||||
0.00276981 4. 0. 0. 0 ! s5*LOG(Ts)^4
|
||||
0.297 0. 0. 0. 0 ! e3^2*EXP(above)
|
||||
2.01588 1. 0. 0. 0 ! e2*T (use below)
|
||||
30.41 0. 0. 0. 0 ! SQRT(e2*T*Tred)
|
||||
!Virial terms
|
||||
0.6022137 30.41 1. 0. 0 !Reducing parameters for eta, T, rho
|
||||
-0.187 0. 0. 0. 0 ! b2
|
||||
2.4871 -1. 0. 0. 0 ! b3/Ts
|
||||
3.7151 -2. 0. 0. 0 ! b4/Ts^2
|
||||
-11.0972 -3. 0. 0. 0 ! b5/Ts^3
|
||||
9.0965 -4. 0. 0. 0 ! b6/Ts^4
|
||||
-3.8292 -5. 0. 0. 0 ! b7/Ts^5
|
||||
0.5166 -6. 0. 0. 0 ! b8/Ts^6
|
||||
0.297 0. 0. 0. 0 ! b9^3*sum(above)
|
||||
!Residual function terms
|
||||
1000. 33.145 45.096479408 0. 0 !Reducing parameters for eta, T, rho
|
||||
0.0456334068 1. 0. 0. 0 ! a2*Tr
|
||||
0.232797868 -1. 0. 0. 0 ! a3/Tr
|
||||
0.363576595 0. 6. 0. 0 ! a6*Dr^6
|
||||
0.958326120 0. 2. 0. 0 ! a4*Dr^2
|
||||
0.127941189 0. 0. 0. 0 ! a5
|
||||
1.0 1. 0. 0. 0 ! [a4*Dr^2 from above]/(a5+Tr)
|
||||
0.00643449673 0. 2. 0. 0 ! a1*Dr^2*EXP(above)
|
||||
NUL !Pointer to the viscosity critical enhancement auxiliary function (none used)
|
||||
|
||||
|
||||
|
||||
|
||||
================================================================================
|
||||
|
||||
#TCX !---Thermal conductivity---
|
||||
TC1 !Pure fluid thermal conductivity model for hydrogen (normal) of Assael et al. (2011).
|
||||
:DOI: 10.1063/1.3606499
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Assael, M.J., Assael, J.-A.M., Huber, M.L., Perkins, R.A., and Takata, Y.,
|
||||
? "Correlation of the Thermal Conductivity of Normal and Parahydrogen
|
||||
? from the Triple Point to 1000 K and up to 100 MPa,"
|
||||
? J. Phys. Chem. Ref. Data, 40(3), 033101, 2011.
|
||||
?
|
||||
?The estimated uncertainty is less than 4% from 100 K to 1000 K at pressures to 100 MPa.
|
||||
? For temperatures from the triple point to 100 K, at pressures
|
||||
? to 12 MPa, we estimate the uncertainty to be 7%, except near the critical point.
|
||||
? The model behaves in a physically reasonable manner for extrapolations to pressures above
|
||||
? 12 MPa at temperatures below 100 K, but will be subject to larger uncertainties.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
1000.0 !Upper temperature limit [K]
|
||||
2000000.0 !Upper pressure limit [kPa]
|
||||
102.0 !Maximum density [mol/L]
|
||||
7 4 !# terms for dilute gas function: numerator, denominator
|
||||
1.0 0.001 !Reducing parameters for T, tcx
|
||||
-12415900. 0.
|
||||
5040560. 1.
|
||||
-48086.8 2.
|
||||
326.394 3.
|
||||
0.0956218 4.
|
||||
1.73488e-4 5.
|
||||
-3.12802e-8 6.
|
||||
5043050. 0.
|
||||
-24375.3 1.
|
||||
151.523 2.
|
||||
1.0 3.
|
||||
10 0 !# terms for background gas function: numerator, denominator
|
||||
33.145 15.508 1. !Reducing parameters for T, rho, tcx
|
||||
0.0363081 0. 1. 0.
|
||||
-0.0207629 0. 2. 0.
|
||||
0.031481 0. 3. 0.
|
||||
-0.0143097 0. 4. 0.
|
||||
0.0017498 0. 5. 0.
|
||||
0.0018337 1. 1. 0.
|
||||
-0.00886716 1. 2. 0.
|
||||
0.015826 1. 3. 0.
|
||||
-0.0106283 1. 4. 0.
|
||||
0.00280673 1. 5. 0.
|
||||
TK3 !Pointer to critical enhancement auxiliary function
|
||||
|
||||
|
||||
#AUX !---Auxiliary function for the thermal conductivity critical enhancement
|
||||
TK3 !Simplified thermal conductivity critical enhancement for hydrogen (normal) of Assael et al. (2011).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Assael, M.J., Assael, J.-A.M., Huber, M.L., Perkins, R.A., and Takata, Y., 2011.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
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)
|
||||
1.2415 !Gamma (universal exponent)
|
||||
1.01 !R0 (universal amplitude)
|
||||
0.065 !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)
|
||||
0.15e-9 !Xi0 (amplitude) [m]
|
||||
0.052 !Gam0 (amplitude) [-]
|
||||
0.4e-9 !Qd_inverse (modified effective cutoff parameter) [m]
|
||||
49.7175 !Tref (reference temperature) [K]
|
||||
|
||||
|
||||
|
||||
|
||||
********************************************************************************
|
||||
|
||||
@ETA !---Viscosity---
|
||||
VS4 !Pure fluid generalized friction theory viscosity model for hydrogen (normal) of Quinones-Cisneros et al. (2011).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Quinones-Cisneros, S.E. and Deiters, U.K.,
|
||||
? model of 1-march-2011 unpublished
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
2000.0 !Upper temperature limit [K]
|
||||
2000000.0 !Upper pressure limit [kPa]
|
||||
102.0 !Maximum density [mol/L]
|
||||
8 1 2 0 0 0 !Number of terms associated with dilute-gas function
|
||||
NUL !Pointer to reduced effective collision cross-section model; not used
|
||||
0.2827 !Lennard-Jones coefficient sigma [nm];not used
|
||||
59.7 !Lennard-Jones coefficient epsilon/kappa [K];not used
|
||||
33.145 1.0 !Reducing parameters for T, eta
|
||||
0.0 0.5 !Chapman-Enskog term; not used here
|
||||
7.246400680522131 0.0
|
||||
-35.23929484813708 0.25
|
||||
66.45332385860778 0.50
|
||||
-56.674979475607415 0.75
|
||||
26.566570031561248 1.00
|
||||
-5.481307488054635 1.25
|
||||
0.4595978383724549 1.50
|
||||
1. 0.75 !Additional special terms for numerator
|
||||
1. 0.0 !Additional special terms for denominator
|
||||
1. 1.0 !Additional special terms for denominator
|
||||
7 !Number of terms for initial density dependence
|
||||
1.0 0.0157768 !Reducing parameters for T (= eps/k), etaB2 (= 0.6022137*sigma**3)
|
||||
-0.187 0.0 !Coefficient, power in T* = T/(eps/k)
|
||||
75.6327 -1.0
|
||||
3435.61 -2.0
|
||||
-312078. -3.0
|
||||
7779290. -4.0
|
||||
-99584100. -5.0
|
||||
408557000. -6.0
|
||||
-0.02348389676311179 0.02197232806029717 0.0024547322430816313 3.9791170684039065e-8 0.004581319859008102 ! a(0),a(1),a(2)
|
||||
0.026869839733943842 0.027387647542474032 0.013065230652860072 3.0723581102227345e-7 -0.07033089468735152 ! b(0),b(1),b(2)
|
||||
0.0 0.0 0.0 0.0 0.0 ! c(0),c(1),c(2)
|
||||
-3.912305916140789e-5 -2.1198288980972056e-6 4.690087618888682e-6 1.6938783854559677e-11 9.39021777998824e-5 ! A(0),A(1),A(2)
|
||||
-6.381148168720446e-5 5.178086941554603e-4 -4.5508093750991845e-5 -1.3780811004280076e-9 -3.7679840470735697e-4 ! B(0),B(1),B(2)
|
||||
0.0 0.0 0.0 0.0 0.0 ! C(0),C(1),C(2)
|
||||
4.3699367404316626e-7 0.0 -1.1321685281996792e-8 0.0 0.0 ! D(0),D(1),D(2)
|
||||
0.0 0.0 0.0 0.0 0.0 ! E(0),E(1),E(2)
|
||||
NUL !Pointer to the viscosity critical enhancement auxiliary function (none used)
|
||||
|
||||
|
||||
@ETA !---Viscosity---
|
||||
VS1 !Pure fluid viscosity model for hydrogen (normal) of Vargaftik et al. (1996).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Vargaftik, N.B., Vinogradov, Y.K. and Yargin, V.S.
|
||||
? "Handbook of Physical Properties of Liquids and Gases", Begell House, NY 1996
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
2000.0 !Upper temperature limit [K]
|
||||
2000000.0 !Upper pressure limit [kPa]
|
||||
102.0 !Maximum density [mol/L]
|
||||
9 !Number of terms associated with dilute-gas function
|
||||
NUL !Pointer to reduced effective collision cross-section model
|
||||
0.2827 !Lennard-Jones coefficient sigma [nm];not used
|
||||
59.7 !Lennard-Jones coefficient epsilon/kappa [K];not used
|
||||
32.938 1.0 !Reducing parameters for T, eta
|
||||
0.0 0.5 !Chapman-Enskog term; not used here
|
||||
-0.21505 -1.5
|
||||
1.0727 -1.0
|
||||
-1.6935 -0.5
|
||||
0.0 0.0
|
||||
2.2702 0.5
|
||||
0.22123 1.0
|
||||
0.034163 1.5
|
||||
-0.0043206 2.0
|
||||
0 !Number of terms for initial density dependence
|
||||
0 12 0 0 0 0 !# resid terms: close-packed density; simple poly; numerator of rational poly; denominator of rat. poly; numerator of exponential; denominator of exponential
|
||||
32.938 15.556 1.0 !Reducing parameters for T (= eps/k), rho, eta
|
||||
-0.922703 0.0 1. 0. 0 !Powers of tau, del, del0; power of del in exponential [0 indicated no exponential term present]
|
||||
6.41602 -1.0 1. 0. 0
|
||||
-5.98018 -2.0 1. 0. 0
|
||||
0.289715 -3.0 1. 0. 0
|
||||
2.36429 0.0 2. 0. 0
|
||||
-0.27887 0.0 3. 0. 0
|
||||
-11.0595 -1.0 3. 0. 0
|
||||
11.1582 -2.0 3. 0. 0
|
||||
7.18928 -1.0 4. 0. 0
|
||||
-7.76971 -2.0 4. 0. 0
|
||||
-1.21827 -1.0 5. 0. 0
|
||||
1.47193 -2.0 5. 0. 0
|
||||
NUL !Pointer to the viscosity critical enhancement auxiliary function (none used)
|
||||
|
||||
|
||||
|
||||
|
||||
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
|
||||
|
||||
@TRN !---ECS Transport---
|
||||
ECS !Extended Corresponding States model (Nitrogen reference); predictive mode for hydrogen (normal).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Klein, S.A., McLinden, M.O., and Laesecke, A., "An Improved Extended Corresponding States Method for Estimation of Viscosity of Pure Refrigerants and Mixtures," Int. J. Refrigeration, 20(3):208-217, 1997. doi: 10.1016/S0140-7007(96)00073-4.
|
||||
?McLinden, M.O., Klein, S.A., and Perkins, R.A., "An Extended Corresponding States Model for the Thermal Conductivity of Refrigerants and Refrigerant Mixtures," Int. J. Refrigeration, 23(1):43-63, 2000. doi: 10.1016/S0140-7007(99)00024-9
|
||||
?
|
||||
?The Lennard-Jones parameters were taken from Reid, R.C., Prausnitz, J.M., and Poling, B.E., "The Properties of Gases and Liquids," 4th edition, New York, McGraw-Hill Book Company, 1987.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
500.0 !Upper temperature limit [K]
|
||||
40000.0 !Upper pressure limit [kPa]
|
||||
38.148 !Maximum density [mol/L]
|
||||
FEQ NITROGEN.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)
|
||||
0.2827 !Lennard-Jones coefficient sigma [nm] for ECS method
|
||||
59.7 !Lennard-Jones coefficient epsilon/kappa [K] for ECS method
|
||||
1 0 0 !Number of terms in f_int term in Eucken correlation, spare1, spare2
|
||||
0.00132 0. 0. 0. !Coefficient, power of T, spare1, spare2
|
||||
1 0 0 !Number of terms in psi (visc shape factor): poly,spare1,spare2
|
||||
1.0 0. 0. 0. !Coefficient, power of Tr, power of Dr, spare
|
||||
1 0 0 !Number of terms in chi (t.c. shape factor): poly,spare1,spare2
|
||||
1.0 0. 0. 0. !Coefficient, power of Tr, power of Dr, spare
|
||||
TK3 !Pointer to critical enhancement auxiliary function
|
||||
|
||||
|
||||
|
||||
|
||||
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
|
||||
|
||||
#STN !---Surface tension---
|
||||
ST1 !Surface tension model for hydrogen (normal) 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. !
|
||||
3 !Number of terms in surface tension model
|
||||
33.145 !Critical temperature used in fit (dummy)
|
||||
-1.4165 0.63882 !Sigma0 and n
|
||||
0.746383 0.659804
|
||||
0.675625 0.619149
|
||||
|
||||
|
||||
#DE !---Dielectric constant---
|
||||
DE3 !Dielectric constant model for hydrogen (normal) of Harvey and Lemmon (2005).
|
||||
:DOI: 10.1007/s10765-005-2351-5
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Harvey, A.H. and Lemmon, E.W.,
|
||||
? "Method for Estimating the Dielectric Constant of Natural Gas Mixtures,"
|
||||
? Int. J. Thermophys., 26(1):31-46, 2005. doi: 10.1007/s10765-005-2351-5
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
0. !
|
||||
10000. !
|
||||
0. !
|
||||
0. !
|
||||
273.16 1000.0 1.0 !Reducing parameters for T and D
|
||||
0 2 3 0 0 0 !Number of terms in dielectric constant model
|
||||
2.0306 0. 1. 0. !Coefficient, T exp, D exp
|
||||
0.0056 1. 1. 0.
|
||||
0.181 0. 2. 0.
|
||||
0.021 1. 2. 0.
|
||||
-7.4 0. 3. 0.
|
||||
|
||||
|
||||
#MLT !---Melting line---
|
||||
ML1 !Melting line model for normal hydrogen
|
||||
:DOI:
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Preliminary equation, 2007.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
400.0 !Upper temperature limit [K]
|
||||
0. !
|
||||
0. !
|
||||
13.957 7.3578 !Reducing temperature and pressure
|
||||
1 2 0 0 0 0 !Number of terms in melting line equation
|
||||
1.0 0.0 !Coefficients and exponents
|
||||
5626.3 1.0
|
||||
2717.2 1.83
|
||||
|
||||
|
||||
#SBL !---Sublimation line---
|
||||
SB3 !Sublimation line model for hydrogen (normal) of Lemmon (2003).
|
||||
:DOI:
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Lemmon, E.W., 2003.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
0. !
|
||||
13.957 !Upper temperature limit [K]
|
||||
0. !
|
||||
0. !
|
||||
13.957 7.70 !Reducing temperature and pressure
|
||||
0 1 0 0 0 0 !Number of terms in sublimation line equation
|
||||
-8.065 0.93 !Coefficients and exponents
|
||||
|
||||
|
||||
#PS !---Vapor pressure---
|
||||
PS5 !Vapor pressure equation for hydrogen (normal) of Leachman et al. (2009).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?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. !
|
||||
33.145 1296.4 !Reducing parameters
|
||||
4 0 0 0 0 0 !Number of terms in equation
|
||||
-4.89789 1.0
|
||||
0.988558 1.5
|
||||
0.349689 2.0
|
||||
0.499356 2.85
|
||||
|
||||
|
||||
#DL !---Saturated liquid density---
|
||||
DL1 !Saturated liquid density equation for hydrogen (normal) of Lemmon (2010).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Lemmon, C.K. and Lemmon, E.W., 2010.
|
||||
?
|
||||
?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. !
|
||||
33.145 15.508 !Reducing parameters
|
||||
5 0 0 0 0 0 !Number of terms in equation
|
||||
15.456 0.62
|
||||
-41.720 0.83
|
||||
50.276 1.05
|
||||
-27.947 1.3
|
||||
5.6718 1.6
|
||||
|
||||
|
||||
#DV !---Saturated vapor density---
|
||||
DV3 !Saturated vapor density equation for hydrogen (normal) of Lemmon (2010).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Lemmon, C.K. and Lemmon, E.W., 2010.
|
||||
?
|
||||
?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. !
|
||||
33.145 15.508 !Reducing parameters
|
||||
6 0 0 0 0 0 !Number of terms in equation
|
||||
-2.9962 0.466
|
||||
-16.724 2.0
|
||||
15.819 2.4
|
||||
-16.852 4.0
|
||||
34.586 7.0
|
||||
-53.754 8.0
|
||||
|
||||
|
||||
@END
|
||||
c 1 2 3 4 5 6 7 8
|
||||
c2345678901234567890123456789012345678901234567890123456789012345678901234567890
|
||||
|
||||
|
||||
@ETA !Viscosity model specification
|
||||
VS0 pure fluid viscosity model of McCarty and Weber (1972).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?McCarty, R.D. and Weber, L.A.,
|
||||
? "Thermophysical properties of parahydrogen from the freezing liquid line to
|
||||
? 5000 R for pressures to 10,000 psia,"
|
||||
? Natl. Bur. Stand., Tech. Note 617, 1972.
|
||||
?
|
||||
?The uncertainty in viscosity ranges from 4% to 15%.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
1000.0 !Upper temperature limit [K]
|
||||
121000.0 !Upper pressure limit [kPa]
|
||||
43.0 !Maximum density [mol/L]
|
||||
H2 !Pointer to hardcoded thermal conductivity model
|
||||
0 9 8 0 0 0 0 0 !Number of terms for various pieces
|
||||
1.0 1.0 1.0 !Reducing parameters for T, rho, eta
|
||||
-18.41091042788 0. 0. 0. 0 !Dilute gas coeffs
|
||||
31.85762039455 0. 0. 0. 0
|
||||
-23.08233586574 0. 0. 0. 0
|
||||
9.129812714730 0. 0. 0. 0
|
||||
-2.163626387630 0. 0. 0. 0
|
||||
0.3175128582601 0. 0. 0. 0
|
||||
-0.02773173035271 0. 0. 0. 0
|
||||
0.001347359367871 0. 0. 0. 0
|
||||
-0.2775671778154e-4 0. 0. 0. 0
|
||||
-13.24266117873 0. 0. 0. 0 !Residual coeffs
|
||||
18.95048470537 0. 0. 0. 0
|
||||
21.84151514282 0. 0. 0. 0
|
||||
97718.27164811 0. 0. 0. 0
|
||||
-1157.010275059 0. 0. 0. 0
|
||||
191.1147702539 0. 0. 0. 0
|
||||
-3186.427506942 0. 0. 0. 0
|
||||
0.0705565 0. 0. 0. 0
|
||||
NUL !Pointer to the viscosity critical enhancement auxiliary function (none used)
|
||||
|
||||
|
||||
@ETA !Viscosity model specification
|
||||
VS0 pure fluid viscosity model from symbolic regression (Muzny, Huber, Kazakov) (2013).
|
||||
?
|
||||
?```````````````````````````````````````````````````````````````````````````````
|
||||
?Muzny, C.D., Huber, M.L., and Kazakov, A.F.,
|
||||
? "Correlation for the Viscosity of normal hydrogen obtained from symbolic regression"
|
||||
? J. Chem. Eng. Data, 2013. 58. 969-979.
|
||||
?
|
||||
?The estimated uncertainty is 4 % for the saturated liquid from the triple point to 31 K, with larger deviations
|
||||
? as the critical region is approached. The estimated uncertainty is 4 % for the supercritical fluid phase at pressures to 200 MPa.
|
||||
? For the limited range of 200 K to 400 K at pressures up to 0.1 MPa, the uncertainty is 0.1 %.
|
||||
?
|
||||
!```````````````````````````````````````````````````````````````````````````````
|
||||
13.957 !Lower temperature limit [K]
|
||||
2000.0 !Upper temperature limit [K]
|
||||
2000000.0 !Upper pressure limit [kPa]
|
||||
102.0 !Maximum density [mol/L]
|
||||
H2A !Pointer to hardcoded model
|
||||
0 0 0 0 0 0 0 0 !Number of terms for various pieces
|
||||
1.0 1.0 1.0 !Reducing parameters for T, rho, eta
|
||||
NUL !Pointer to the viscosity critical enhancement auxiliary function (none used)
|
||||
Reference in New Issue
Block a user