These tables give thermodynamic and transport properties of a variety of fluids, as generated from the correlations presented in the references below. The properties tabulated are defined in the table below. All extensive properties are given on a mass basis. Not all properties are included for every substance. The references should be consulted for information on the uncertainties. Column definitions for the tables are as follows.
Column heading | Definition |
T | Temperature, in K |
P | Pressure, in units of MPa |
ρ | Density, in units of kg m-3 |
H | Enthalpy, in units of kJ kg-1 |
S | Entropy, in units of kJ kg-1 K-1 |
Cv | Isochoric heat capacity, in units of kJ kg-1 K-1 |
Cp | Isobaric heat capacity, in units of kJ kg-1 K-1 |
u | Speed of sound, in units of m s-1 |
η | Viscosity, in units of μPa s |
λ | Thermal conductivity, in units of mW m-1 K-1 |
D | Static dielectric constant, dimensionless |
Values are given first along the saturation line. The first two rows are the properties at the triple point. The final row gives the properties at the critical point. Two rows are given for each temperature (except at the critical point); the first row gives the values of the liquid phase (note the high density), and the second row gives the values of the vapor phase (lower densities). Following the saturation tables, values are given as a function of temperature for several isobars. A duplicate entry in the isobar section indicates a phase transition (liquid–vapor) at that temperature; property values are then given for both phases. The phase can be determined by noting the sharp decrease in density between two successive temperature entries; all rows above this point refer to the liquid phase, and all rows below refer to the gas phase. If there is no sharp discontinuity in density, all data in the table refer to the supercritical region (i.e., the isobar is above the critical pressure). If the first temperature in the isobars is not an integer, this state point refers to the properties of the liquid at the melting line. All temperatures are given on ITS-90, except those for oxygen, where the equation of state still uses the IPTS-68 temperature scale.
Properties for each fluids are given in individual tables as shown below. Reference state information is included.
Table no. | Fluid name | Fluid mol. form. | Reference state |
1 | Nitrogen | N2 | Zero enthalpy in the gas phase at 0 K |
2 | Oxygen | O2 | Zero enthalpy in the gas phase at 0 K |
3 | Argon | Ar | Zero enthalpy in the gas phase at 0 K |
4 | paraHydrogen | H2 (para) | Zero enthalpy and entropy at the saturated liquid state at the normal boiling point |
5 | Helium | 4He | Zero enthalpy and entropy at the saturated liquid state at the normal boiling point |
6 | Methane | CH4 | Zero enthalpy and entropy at the saturated liquid state at the normal boiling point |
7 | Ethane | C2H6 | Zero enthalpy and entropy at the saturated liquid state at the normal boiling point |
8 | Propane | C3H8 | Enthalpy = 200 kJ kg–1 and entropy = 1 kJ kg–1 K–1 at –40 °C |
9 | Carbon dioxidw | CO2 | Enthalpy = 200 kJ kg–1 and entropy = 1 kJ kg–1 K–1 at –40 °C |
Additional calculations at state points not listed below and for fluids not contained here can be obtained with the use of the NIST Standard Reference Data program REFPROP <http://www.nist.gov/srd/refprop>.
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T/ K | P/ MPa | ρ/ kg m-3 | H/ kJ kg-1 | S/ kJ kg-1 K-1 | Cv/ kJ kg-1 K-1 | Cp/ kJ kg-1 K-1 | u/ m s-1 | η/ μPa s | λ/ mW m-1 K-1 | D |
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Saturation | ||||||||||
63.151 | 0.01252 | 867.2 | -150.7 | 2.426 | 1.176 | 2.000 | 995.3 | 311.6 | 173.3 | 1.47003 |
63.151 | 0.01252 | 0.6743 | 64.78 | 5.838 | 0.7499 | 1.058 | 161.1 | 4.376 | 5.621 | 1.00032 |
70.0 | 0.03854 | 838.5 | -137 | 2.632 | 1.130 | 2.014 | 925.7 | 220.2 | 159.5 | 1.45241 |
70.0 | 0.03854 | 1.896 | 71.10 | 5.605 | 0.7580 | 1.082 | 168.4 | 4.883 | 6.355 | 1.00089 |
80.0 | 0.1369 | 793.9 | -116.6 | 2.903 | 1.069 | 2.056 | 824.4 | 145.1 | 139.6 | 1.42541 |
80.0 | 0.1369 | 6.089 | 79.10 | 5.349 | 0.7773 | 1.145 | 176.7 | 5.652 | 7.506 | 1.00286 |
90.0 | 0.3605 | 745.0 | -95.52 | 3.147 | 1.020 | 2.141 | 719.0 | 102.8 | 119.8 | 1.39622 |
90.0 | 0.3605 | 15.08 | 84.97 | 5.153 | 0.8078 | 1.266 | 181.8 | 6.482 | 8.868 | 1.00710 |
100.0 | 0.7783 | 689.4 | -73.21 | 3.376 | 0.9832 | 2.318 | 605.2 | 75.76 | 100.1 | 1.36351 |
100.0 | 0.7783 | 31.96 | 87.77 | 4.986 | 0.8548 | 1.503 | 183.3 | 7.429 | 10.73 | 1.01510 |
110.0 | 1.466 | 621.5 | -48.49 | 3.601 | 0.9667 | 2.743 | 476.4 | 55.99 | 80.44 | 1.32430 |
110.0 | 1.466 | 62.58 | 85.84 | 4.823 | 0.9284 | 2.062 | 180.8 | 8.626 | 13.83 | 1.02974 |
120.0 | 2.511 | 523.4 | -17.87 | 3.851 | 1.011 | 4.508 | 317.3 | 38.43 | 61.01 | 1.26895 |
120.0 | 2.511 | 125.1 | 74.17 | 4.618 | 1.099 | 4.631 | 172.6 | 10.62 | 21.71 | 1.06012 |
126.192 | 3.396 | 313.3 | 29.23 | 4.215 | 18.30 | 1.15559 | ||||
P = 0.1 MPa (1 bar) | ||||||||||
63.170 | 0.1 | 867.3 | -150.6 | 2.426 | 1.176 | 2.000 | 995.6 | 311.6 | 173.3 | 1.47007 |
77.244 | 0.1 | 806.6 | -122.2 | 2.831 | 1.085 | 2.041 | 852.5 | 161.4 | 145.1 | 1.43304 |
77.244 | 0.1 | 4.556 | 77.07 | 5.412 | 0.7710 | 1.123 | 174.7 | 5.435 | 7.174 | 1.00214 |
80.0 | 0.1 | 4.379 | 80.15 | 5.451 | 0.7666 | 1.112 | 178.3 | 5.623 | 7.443 | 1.00206 |