Thermodynamic relations: Difference between revisions
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These thermodynamic relations are also known as ''coefficient relations''. | <div style="border:1px solid #f3f3ff; padding-left: 0.5em !important; background-color: #f3f3ff; border-width: 0 0 0 1.4em; clear:right; float:right;"> | ||
Notation used: | |||
*<math>H</math> is the [[enthalpy]] | |||
*<math>T</math> is the [[temperature]] | |||
*<math>G</math> is the [[Gibbs energy function]] | |||
*<math>U</math> is the [[internal energy]], | |||
*<math>V</math> is the volume | |||
*<math>A</math> is the [[Helmholtz energy function]] | |||
*<math>p</math> is the [[pressure]] | |||
*<math>S</math> is the [[entropy]] | |||
</div> | |||
These '''thermodynamic relations''' are also known as ''coefficient relations''. | |||
<math>T=\left(\frac{\partial U}{\partial S}\right)_V </math> | <math>T=\left(\frac{\partial U}{\partial S}\right)_V </math> | ||
<math> | <math> p=-\left(\frac{\partial U}{\partial V}\right)_S </math> | ||
<math>T=\left(\frac{\partial H}{\partial S}\right)_p </math> | <math>T=\left(\frac{\partial H}{\partial S}\right)_p </math> | ||
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<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math> | <math> V=\left(\frac{\partial G}{\partial p}\right)_T </math> | ||
==See also== | ==See also== | ||
*[[Maxwell's relations]] | *[[Maxwell's relations]] | ||
*[[Bridgman thermodynamic formulas]] | |||
[[Category: Classical thermodynamics]] | [[Category: Classical thermodynamics]] |
Latest revision as of 15:10, 5 October 2011
Notation used:
- is the enthalpy
- is the temperature
- is the Gibbs energy function
- is the internal energy,
- is the volume
- is the Helmholtz energy function
- is the pressure
- is the entropy
These thermodynamic relations are also known as coefficient relations.