Thermodynamic relations: Difference between revisions

Revision as of 16:31, 23 February 2007

Also known as coefficient relations.

$T = {(\frac{\partial U}{\partial S})}_{V}$

$P = - {(\frac{\partial U}{\partial V})}_{S}$

$T = {(\frac{\partial H}{\partial S})}_{p}$

$V = {(\frac{\partial H}{\partial p})}_{S}$

$S = - {(\frac{\partial F}{\partial T})}_{V}$

$p = - {(\frac{\partial A}{\partial V})}_{T}$

$S = - {(\frac{\partial G}{\partial T})}_{p}$

$V = {(\frac{\partial G}{\partial p})}_{T}$

Revision as of 12:36, 20 February 2007 (edit) Carl McBride (talk \| contribs) m (New page: Also known as coefficient relations. <math>T=\left(\frac{\partial U}{\partial S}\right)_V </math> <math> P=-\left(\frac{\partial U}{\partial V}\right)_S </math> <math>T=\left(\frac{\pa...)		Revision as of 16:31, 23 February 2007 (edit) (undo) Carl McBride (talk \| contribs) mNo edit summary Newer edit →
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	<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>		<math> V=\left(\frac{\partial G}{\partial p}\right)_T </math>
			[[Category: Classical thermodynamics]]