Latest revision as of 14:08, 5 October 2011

{\frac{\partial S}{\partial V} |}_{T} = {\frac{\partial p}{\partial T} |}_{V}

{\frac{\partial T}{\partial p} |}_{S} = {\frac{\partial V}{\partial S} |}_{p}

{\frac{\partial S}{\partial p} |}_{T} = - {\frac{\partial V}{\partial T} |}_{p}

{\frac{\partial T}{\partial V} |}_{S} = - {\frac{\partial p}{\partial S} |}_{V}

where $S$ is the entropy, $V$ is the volume, $T$ is the temperature, $p$ is the pressure

@@ Line 10: / Line 10: @@
 :<math>\left. \frac{\partial T}{\partial V} \right\vert_S  =  - \left. \frac{\partial p}{\partial S} \right\vert_V </math>
+where <math>S</math> is the [[entropy]], <math>V</math> is the volume, <math>T</math> is the [[temperature]], <math>p</math> is the [[pressure]]
 =See also=
 *[[Thermodynamic relations]]
+*[[Bridgman thermodynamic formulas]]
 [[Category: Classical thermodynamics]]

Maxwell's relations: Difference between revisions