Solid-liquid phase transitions: Difference between revisions
		
		
		
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| m (→See also:   Added an internal link to the Lindemann melting law.) | Carl McBride (talk | contribs)  m (→See also:   Changed internal link) | ||
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| ==See also== | ==See also== | ||
| *[[Kosterlitz-Thouless transition]] | *[[Kosterlitz-Thouless transition]] | ||
| *[[Lindemann melting law]] | *[[Melting curve#Lindemann melting law | Lindemann melting law]] | ||
| *[[Spinodal decomposition]] | *[[Spinodal decomposition]] | ||
| *[[Supercooling and nucleation]] | *[[Supercooling and nucleation]] | ||
Revision as of 13:50, 24 June 2011
In a fluid, solid-liquid phase transitions are thought of as being governed mainly by entropy. This is at variance with the gas-liquid phase transition, which is mainly governed by energy.
This point of view is supported by the solid-liquid transition being not being greatly dependent on the temperature, but on the density. Accordingly, the hard sphere fluid, for which temperature does not enter at all, exhibits a fluid-solid transition.
See also
- Kosterlitz-Thouless transition
- Lindemann melting law
- Spinodal decomposition
- Supercooling and nucleation
