Classical thermodynamics: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  No edit summary | ||
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| *[[Gay-Lussac's law]] | *[[Gay-Lussac's law]] | ||
| *[[Gibbs-Duhem relation]] | *[[Gibbs-Duhem relation]] | ||
| *[[Gibbs-Helmholtz equations]] | |||
| *[[Gibbs energy function]] | *[[Gibbs energy function]] | ||
| *[[Helmholtz energy function]] | *[[Helmholtz energy function]] | ||
Revision as of 18:03, 28 May 2007
- Boltzmann constant
- Boyle's law
- Carnot cycle
- Charles's law
- Chemical potential
- Compressibility
- Compressibility factor
- Enthalpy
- First law of thermodynamics
- Gay-Lussac's law
- Gibbs-Duhem relation
- Gibbs-Helmholtz equations
- Gibbs energy function
- Helmholtz energy function
- Maxwell's relations
- Second law of thermodynamics
- Specific heat
- Thermodynamic integration
- Thermodynamic relations
- Zeroth law of thermodynamics