Calculate thermodynamic and electrostatic properties of water.
water(property = NULL, T = get("thermo")$opt$Tr, P = "Psat")
water.props(formulation = get("thermo")$opt$water)
water.SUPCRT92(property, T = 298.15, P = 1)
water.IAPWS95(property, T = 298.15, P = 1)character, name(s) of property(s) to calculate
numeric, temperature (K)
numeric, pressure (bar), or Psat for vapor-liquid saturation
character, name of formulation for which to return names of available properties
For water and water.SUPCRT92 a data frame the number of rows of which corresponds to the number of input temperature, pressure and/or density values.
These functions compute the thermodynamic (Gibbs energy and it derivatives) and electrostatic (dielectric constant and its derivatives) properties of liquid or supercritical using equations of state taken from the literature.
The high-level function water accepts two major computational alternatives.
The default option (i.e., thermo$opt$water equal to SUPCRT92) is retrieve thermodynamic and electrostatic properties as a function of temperature and pressure using a FORTRAN subroutine taken from the SUPCRT92 software package (Johnson et al., 1992).
If thermo$opt$water is set to IAPWS95, the thermodynamic properties are calculated using an implementation in R code of the IAPWS-95 formulation (Wagner and Pruss, 2002), and electrostatic properties are calculated using the equations of Archer and Wang, 1990.
The allowed propertys for water are one or more of those given below, depending on the computational option; availability is shown by an asterisk.
The names of properties in the arguments are not case sensitive. Note that some of the properties that can actually be calculated using the different formulations are not implemented here.
Except for rho, the units are those used by Johnson and Norton, 1991.
| Property | Description | Units | IAPWS95 | SUPCRT92 |
A |
Helmholtz energy | cal mol\(^{-1}\) | * | * |
G |
Gibbs energy | cal mol\(^{-1}\) | * | * |
S |
Entropy | cal K\(^{-1}\) mol\(^{-1}\) | * | * |
U |
Internal energy | cal mol\(^{-1}\) | * | * |
H |
Enthalpy | cal mol\(^{-1}\) | * | * |
Cv |
Isochoric heat capacity | cal K\(^{-1}\) mol\(^{-1}\) | * | * |
Cp |
Isobaric heat capacity | cal K\(^{-1}\) mol\(^{-1}\) | * | * |
Speed |
Speed of sound | cm s\(^{-1}\) | NA | * |
alpha |
Coefficient of isobaric expansivity | K\(^{-1}\) | NA | * |
beta |
Coefficient of isothermal compressibility | bar\(^{-1}\) | NA | * |
diel |
Dielectric constant | dimensionless | NA | * |
visc |
Dynamic viscosity | g cm\(^{-1}\) s\(^{-1}\) | NA | * |
tcond |
Thermal conductivity | cal cm\(^{-1}\) s\(^{-1}\) K\(^{-1}\) | NA | * |
tdiff |
Thermal diffusivity | cm\(^2\) s\(^{-1}\) | NA | * |
Prndtl |
Prandtl number | dimensionless | NA | * |
visck |
Kinematic viscosity | cm\(^2\) s\(^{-1}\) | NA | * |
albe |
Isochoric expansivity | bar K\(^{-1}\) | NA | * |
| -compressibility | ||||
ZBorn |
Z Born function | dimensionless | NA | * |
YBorn |
Y Born function | K\(^{-1}\) | * | * |
QBorn |
Q Born function | bar\(^{-1}\) | * | * |
daldT |
Isobaric temperature derivative | K\(^{-2}\) | NA | * |
| of expansibility | ||||
XBorn |
X Born function | K\(^{-2}\) | * | * |
NBorn |
N Born function | bar\(^{-2}\) | * | NA |
UBorn |
U Born function | bar\(^{-1}\) K\(^{-1}\) | * | NA |
V |
Volume | cm\(^3\) mol\(^{-1}\) | * | * |
rho |
Density | kg cm\(^3\) | * | * |
Psat |
Saturation vapor pressure | bar | * | * |
E |
Isobaric expansivity | cm\(^3\) K\(^{-1}\) | NA | * |
kT |
Isothermal compressibility | cm\(^3\) bar\(^{-1}\) | NA | * |
de.dT |
Temperature derivative | K\(^{-1}\) | * | NA |
| of dielectric constant | ||||
de.dP |
Pressure derivative | bar\(^{-1}\) | * | NA |
| of dielectric constant | ||||
P |
Pressure | bar | * | NA |
water.props returns the names of the available properties listed in this table, reflecting the current setting of thermo$opt$water.
water.SUPCRT92 interfaces to the FORTRAN subroutine taken from the SUPCRT92 package (H2O92D.F) for calculating properties of water.
These calculations are based on data and equations of Levelt-Sengers et al., 1983, Haar et al., 1984, and Johnson and Norton, 1991, among others (see Johnson et al., 1992).
A value of P set to Psat refers to one bar below 100 \(^{\circ}\)C, otherwise to the vapor-liquid saturation pressure at temperatures below the critical point (Psat is not available at temperatures above the critical point).
water.SUPCRT92 provides a limited interface to the FORTRAN subroutine; some functions provided there are not made available here (e.g., using variable density instead of pressure, or calculating the properties of steam).
The properties of steam in CHNOSZ, as in SUPCRT92, are calculated using general equations for crystalline, gaseous and liquid species (cgl).
The stated temperature limits of validity of calculations in water.SUPCRT92 are from the greater of 0 \(^{\circ}\)C or the melting temperature at pressure, to 2250 \(^{\circ}\)C (Johnson et al., 1992).
Valid pressures are from the greater of zero bar or the melting pressure at temperature to 30000 bar.
The present functions do not check these limits and will attempt calculations for any range of input parameters, but may return NA for properties that fail to be calculated at given temperatures and pressures and/or produce warnings or even errors when problems are encountered.
Starting with version 0.9-9.4, a check for minimum pressure (in valTP function in H2O92D.f) has been bypassed so that properties of H2O can be calculated using water.SUPCRT92 at temperatures below the 0.01 \(^{\circ}\)C triple point.
A primary check is still enforced (Tbtm), giving a minimum valid temperature of 253.15 K.
water.IAPWS95 is a wrapper around IAPWS95, rho.IAPWS95 and water.AW90.
water.IAPWS95 provides for calculations at specific temperature and pressure; density, needed for IAPWS95, is inverted from pressure using rho.IAPWS95.
The function also contains routines for calculating the Born functions as numerical derivatives of the static dielectric constant (from water.AW90).
For compatibility with geochemical modeling conventions, the values of Gibbs energy, enthalpy and entropy output by IAPWS95 are converted by water.IAPWS95 to the triple point reference state adopted in SUPCRT92 (Johnson and Norton, 1991; Helgeson and Kirkham, 1974).
water.IAPWS95 also accepts setting P to Psat, with the saturation pressure calculated from WP02.auxiliary; by default the returned properties are for the liquid, but this can be changed to the vapor in thermo$opt$IAPWS.sat.
Archer, D. G. and Wang, P. M. (1990) The dielectric constant of water and Debye-Huckel limiting law slopes. J. Phys. Chem. Ref. Data 19, 371--411. https://doi.org/10.1063/1.555853
Haar, L., Gallagher, J. S. and Kell, G. S. (1984) NBS/NRC Steam Tables. Hemisphere, Washington, D. C., 320 p. http://www.worldcat.org/oclc/301304139
Helgeson, H. C. and Kirkham, D. H. (1974) Theoretical prediction of the thermodynamic behavior of aqueous electrolytes at high pressures and temperatures. I. Summary of the thermodynamic/electrostatic properties of the solvent. Am. J. Sci. 274, 1089--1098. http://www.ajsonline.org/cgi/content/abstract/274/10/1089
Johnson, J. W. and Norton, D. (1991) Critical phenomena in hydrothermal systems: state, thermodynamic, electrostatic, and transport properties of H\(_2\)O in the critical region. Am. J. Sci. 291, 541--648. http://www.ajsonline.org/cgi/content/abstract/291/6/541
Johnson, J. W., Oelkers, E. H. and Helgeson, H. C. (1992) SUPCRT92: A software package for calculating the standard molal thermodynamic properties of minerals, gases, aqueous species, and reactions from 1 to 5000 bar and 0 to 1000\(^{\circ}\)C. Comp. Geosci. 18, 899--947. https://doi.org/10.1016/0098-3004(92)90029-Q
Levelt-Sengers, J. M. H., Kamgarparsi, B., Balfour, F. W. and Sengers, J. V. (1983) Thermodynamic properties of steam in the critical region. J. Phys. Chem. Ref. Data 12, 1--28. https://doi.org/10.1063/1.555676
Wagner, W. and Pruss, A. (2002) The IAPWS formulation 1995 for the thermodynamic properties of ordinary water substance for general and scientific use. J. Phys. Chem. Ref. Data 31, 387--535. https://doi.org/10.1063/1.1461829
Equations for thermodynamic properties of species other than water are coded in hkf and cgl.
# NOT RUN {
## calculations along saturation curve
T <- seq(273.15, 623.15, 25)
# liquid density, from SUPCRT92
water("rho", T=T, P="Psat")
# values of the saturation pressure, Gibbs energy
water(c("Psat", "G"), T=T, P="Psat")
# derivatives of the dielectric constant (Born functions)
water(c("QBorn", "YBorn", "XBorn"), T=T, P="Psat")
# now at constant pressure
water(c("QBorn", "YBorn", "XBorn"), T=T, P=2000)
## comparing the formulations
T <- convert(c(25, 100, 200, 300), "K")
# IAPWS-95
thermo$opt$water <<- "IAPWS95"
water(water.props(), T=T)
# SUPCRT92 (the default)
thermo$opt$water <<- "SUPCRT92"
water(water.props(), T=T)
## calculating Q Born function
# after Table 22 of Johnson and Norton, 1991
thermo$opt$water <<- "SUPCRT92"
T <- rep(c(375, 400, 425, 450, 475), each=5)
P <- rep(c(250, 300, 350, 400, 450), 5)
w <- water("QBorn", T=convert(T, "K"), P=P)
# the rest is to make a neat table
w <- as.data.frame(matrix(w[[1]], nrow=5))
colnames(w) <- T[1:5*5]
rownames(w) <- P[1:5]
print(w)
# }
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