Tait equation of state: Difference between revisions
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(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
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \kappa_T := \frac{-1}{V} \left ( \frac{\partial V}{\partial p} \right )_T = \frac{1}{V} \frac{C}{B+p}}
or in the integrated form
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle V = V_0 - C \log \frac{B+p}{B+p_0}}
where
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \kappa_T} is the Isothermal compressibility
- is the specific volume.
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle B \ } and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle C \ } 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)