Vapour pressure of water

Vapor pressure of water (0–100 °C)
T, °CT, °FP, kPaP, torrP, atm
0320.61134.58510.0060
5410.87266.54500.0086
10501.22819.21150.0121
15591.705612.79310.0168
20682.338817.54240.0231
25773.169023.76950.0313
30864.245531.84390.0419
35955.626742.20370.0555
401047.381455.36510.0728
451139.589871.92940.0946
5012212.344092.58760.1218
5513115.7520118.14970.1555
6014019.9320149.50230.1967
6514925.0220187.68040.2469
7015831.1760233.83920.3077
7516738.5630289.24630.3806
8017647.3730355.32670.4675
8518557.8150433.64820.5706
9019470.1170525.92080.6920
9520384.5290634.01960.8342
100212101.3200759.96251.0000

The vapor pressure of water is the pressure exerted by molecules of water vapor in gaseous form (whether pure or in a mixture with other gases such as air). The saturation vapor pressure is the pressure at which water vapor is in thermodynamic equilibrium with its condensed state. At pressures higher than saturation vapor pressure, water will condense, while at lower pressures it will evaporate or sublimate. The saturation vapor pressure of water increases with increasing temperature and can be determined with the Clausius–Clapeyron relation. The boiling point of water is the temperature at which the saturated vapor pressure equals the ambient pressure. Water supercooled below its normal freezing point has a higher vapor pressure than that of ice at the same temperature and is, thus, unstable.

Calculations of the (saturation) vapor pressure of water are commonly used in meteorology. The temperature-vapor pressure relation inversely describes the relation between the boiling point of water and the pressure. This is relevant to both pressure cooking and cooking at high altitudes. An understanding of vapor pressure is also relevant in explaining high altitude breathing and cavitation.