This page provides supplementary data to the article properties of water.
Further comprehensive authoritative data can be found at the NIST Chemistry WebBook page on thermophysical properties of fluids.
Vapor pressure formula for steam in equilibrium with liquid water:
where P is equilibrium vapor pressure in kPa, and T is temperature in kelvins.
For T = 273 K to 333 K: A = 7.2326; B = 1750.286; C = 38.1.
For T = 333 K to 423 K: A = 7.0917; B = 1668.21; C = 45.1.
Data in the table above is given for waterâÂÂsteam equilibria at various temperatures over the entire temperature range at which liquid water can exist. Pressure of the equilibrium is given in the second column in kPa. The third column is the heat content of each gram of the liquid phase relative to water at 0 ðC. The fourth column is the heat of vaporization of each gram of liquid that changes to vapor. The fifth column is the work PÃÂV done by each gram of liquid that changes to vapor. The sixth column is the density of the vapor.
Data obtained from CRC Handbook of Chemistry and Physics 44th ed., p. 2390.
<sup>â¡</sup><small>Ice XI triple point is theoretical and has never been obtained</small>
Note: àis density, n is refractive index at 589 nm, and ÷ is viscosity, all at 20 ðC; T<sub>eq</sub> is the equilibrium temperature between two phases: ice/liquid solution for T<sub>eq</sub> < 0âÂÂ0.1 ðC and NaCl/liquid solution for T<sub>eq</sub> above 0.1 ðC.
The data that follows was copied and translated from the German language Wikipedia version of this page (which has moved to here). It provides supplementary physical, thermodynamic, and vapor pressure data, some of which is redundant with data in the tables above, and some of which is additional.
In the following tables, values are temperature-dependent and to a lesser degree pressure-dependent, and are arranged by state of aggregation (s = solid, lq = liquid, g = gas), which are clearly a function of temperature and pressure. All of the data were computed from data given in "Formulation of the Thermodynamic Properties of Ordinary Water Substance for Scientific and General Use" (IAPWS , 1984) (obsolete as of 1995). This applies to:
In the following table, material data are given for standard pressure of 0.1 MPa (equivalent to 1 bar). Up to 99.63 ðC (the boiling point of water at 0.1 MPa), at this pressure water exists as a liquid. Above that, it exists as water vapor. Note that the boiling point of 100.0 ðC is at a pressure of 0.101325 MPa (1 atm), which is the average atmospheric pressure.
In the following table, material data are given with a pressure of 611.7 Pa (equivalent to 0.006117 bar). Up to a temperature of 0.01 ðC, the triple point of water, water normally exists as ice, except for supercooled water, for which one data point is tabulated here. At the triple point, ice can exist together with both liquid water and vapor. At higher temperatures, the data are for water vapor only.
The following table is based on different, complementary sources and approximation formulas, whose values are of various quality and accuracy. The values in the temperature range of âÂÂ100 ðC to 100 ðC were inferred from D. Sunday (1982) and are quite uniform and exact. The values in the temperature range of the boiling point of water up to the critical point (100 ðC to 374 ðC) are drawn from different sources and are substantially less accurate; hence they should be used only as approximate values.
To use the values correctly, consider the following points:
The table values for âÂÂ100 ðC to 100 ðC were computed by the following formulas, where T is in kelvins and vapor pressures, P<sub>w</sub> and P<sub>i</sub>, are in pascals.
Over liquid water
For temperature range: 173.15 K to 373.15 K or equivalently âÂÂ100 ðC to 100 ðC
Over ice
For temperature range: 173.15 K to 273.15 K or equivalently âÂÂ100 ðC to 0 ðC
At triple point
An important basic value, which is not registered in the table, is the saturated vapor pressure at the triple point of water. The internationally accepted value according to measurements of Guildner, Johnson and Jones (1976) amounts to:
Accepted standardized value of the magnetic susceptibility of water at 20 ðC (room temperature) is âÂÂ12.97 cm<sup>3</sup>/mol.
Accepted standardized value of the magnetic susceptibility of water at 20 ðC (room temperature) is âÂÂ0.702 cm<sup>3</sup>/g.