Second law of thermodynamics: Difference between revisions
Jump to navigation
Jump to search
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