Gibbs-Helmholtz equations: Difference between revisions
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Carl McBride (talk | contribs) (New page: :<math>H = -T^2 \left. \frac{\partial (G/T)}{\partial T} \right\vert_p</math> :<math>U = -T^2 \left. \frac{\partial (A/T)}{\partial T} \right\vert_V</math> where *<math>H</math> is the...) |
Carl McBride (talk | contribs) No edit summary |
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*<math>T</math> is the temperature | *<math>T</math> is the temperature | ||
*<math>G</math> is the [[Gibbs energy function]] | *<math>G</math> is the [[Gibbs energy function]] | ||
*<math>U</math> is the [[ | *<math>U</math> is the [[internal energy]], | ||
*<math>V</math> is the volume | *<math>V</math> is the volume | ||
*<math>A</math> is the [[Helmholtz energy function]]. | *<math>A</math> is the [[Helmholtz energy function]]. | ||
Revision as of 17:33, 7 June 2007
where
- is the enthalpy
- is the temperature
- is the Gibbs energy function
- is the internal energy,
- is the volume
- is the Helmholtz energy function.
