Clausius-Clapeyron relation: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) (New page: Upon a phase equilibrium curve :<math>\frac{dp}{dT} = \frac{\Delta \left( \frac{S}{N}\right)}{\Delta \left( \frac{V}{N}\right)} = \frac{\Delta S}{\Delta V}</math> where ''p'' is the [[pr...) |
Carl McBride (talk | contribs) No edit summary |
||
Line 1: | Line 1: | ||
Upon a phase equilibrium curve | The '''Clausius-Clapeyron relation''' is named after [[Rudolf Julius Emanuel Clausius]] and [[Benoît Paul Émile Clapeyron]]. Upon a phase equilibrium curve | ||
:<math>\frac{dp}{dT} = \frac{\Delta \left( \frac{S}{N}\right)}{\Delta \left( \frac{V}{N}\right)} = \frac{\Delta S}{\Delta V}</math> | :<math>\frac{dp}{dT} = \frac{\Delta \left( \frac{S}{N}\right)}{\Delta \left( \frac{V}{N}\right)} = \frac{\Delta S}{\Delta V}</math> |
Latest revision as of 11:43, 26 July 2007
The Clausius-Clapeyron relation is named after Rudolf Julius Emanuel Clausius and Benoît Paul Émile Clapeyron. Upon a phase equilibrium curve
where p is the pressure, T is the temperature, S is the entropy and V is the volume.