Maxwell's relations: Difference between revisions

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(New page: :<math>\left. \frac{\partial S}{\partial V} \right\vert_T = \left. \frac{\partial p}{\partial T} \right\vert_V </math> :<math>\left. \frac{\partial T}{\partial p} \right\vert_S = \le...)
 
m (Defined variables)
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:<math>\left. \frac{\partial T}{\partial V} \right\vert_S  =  - \left. \frac{\partial p}{\partial S} \right\vert_V </math>
:<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=
=See also=
*[[Thermodynamic relations]]
*[[Thermodynamic relations]]
[[Category: Classical thermodynamics]]
[[Category: Classical thermodynamics]]

Revision as of 17:21, 29 January 2008





where is the entropy, is the volume, is the temperature, is the pressure

See also