Second law of thermodynamics: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  m (Added See also section) | ||
| Line 16: | Line 16: | ||
| :<math>dU=\left(\frac{\partial U}{\partial S}\right)_V dS + \left(\frac{\partial U}{\partial V}\right)_S dV</math> | :<math>dU=\left(\frac{\partial U}{\partial S}\right)_V dS + \left(\frac{\partial U}{\partial V}\right)_S dV</math> | ||
| ==See also== | |||
| *[[H-theorem]] | |||
| ==References== | |||
| [[Category: Classical thermodynamics]] | [[Category: Classical thermodynamics]] | ||
Revision as of 14:31, 9 April 2008
For a reversible change
Thus for a closed system ( fixed):
where is the internal energy. For an open system:
where is the chemical potential.
For one has the following total differential