Tait equation of state: Difference between revisions
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Carl McBride (talk | contribs) m (Included page in the water category.) |
(Mention to stiffened equation of state, the two are often confused) |
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*<math> V \ </math> is the [[specific volume]]. | *<math> V \ </math> is the [[specific volume]]. | ||
*<math> B \ </math> and <math> C \ </math> are functions of [[temperature]] that are independent of [[pressure]]. | *<math> B \ </math> and <math> C \ </math> are functions of [[temperature]] that are independent of [[pressure]]. | ||
It is quite common that this name is improperly used for the adiabatic form of the | |||
[[stiffened equation of state]]. | |||
== References == | == References == |
Revision as of 12:23, 10 October 2013
The Tait equation is an equation of state. The equation was originally published by Peter Guthrie Tait in 1888 [1][2]. It may be written as
or in the integrated form
where
- is the Isothermal compressibility
- is the specific volume.
- and are functions of temperature that are independent of pressure.
It is quite common that this name is improperly used for the adiabatic form of the stiffened equation of state.
References
- ↑ P. G. Tait "Report on some of the physical properties of fresh water and sea water", Report on the scientific results of the voyage of H.M.S. Challenger during the years 1873-76. Physics and chemistry 2 pp. 1-76 (1888)
- ↑ Yuan-Hui Li "Equation of state of water and sea water", Journal of Geophysical Research 72 pp. 2665-2678 (1967)