Thermodynamic relations: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  m (Placed notation in a box) | ||
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| These thermodynamic relations are also known as ''coefficient  | <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 H}{\partial p}\right)_S </math> | <math> V=\left(\frac{\partial H}{\partial p}\right)_S </math> | ||
| <math>S=-\left(\frac{\partial  | <math>S=-\left(\frac{\partial A}{\partial T}\right)_V </math> | ||
| <math> p=-\left(\frac{\partial A}{\partial V}\right)_T </math> | <math> p=-\left(\frac{\partial A}{\partial V}\right)_T </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== | |||
| *[[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.