Solid-liquid phase transitions: Difference between revisions
Jump to navigation
Jump to search
No edit summary |
m (→See also: Added an internal link to the Lindemann melting law.) |
||
| Line 8: | Line 8: | ||
==See also== | ==See also== | ||
*[[Kosterlitz-Thouless transition]] | *[[Kosterlitz-Thouless transition]] | ||
*[[Lindemann melting law]] | |||
*[[Spinodal decomposition]] | *[[Spinodal decomposition]] | ||
*[[Supercooling and nucleation]] | *[[Supercooling and nucleation]] | ||
==References== | ==References== | ||
#[http://dx.doi.org/10.1103/RevModPhys.60.161 Katherine J. Strandburg "Two-dimensional melting", Reviews of Modern Physics '''60''' pp. 161-207 (1988)] | #[http://dx.doi.org/10.1103/RevModPhys.60.161 Katherine J. Strandburg "Two-dimensional melting", Reviews of Modern Physics '''60''' pp. 161-207 (1988)] | ||
[[category: phase transitions]] | [[category: phase transitions]] | ||
Revision as of 15:10, 12 May 2009
|
This article is a 'stub' page, it has no, or next to no, content. It is here at the moment to help form part of the structure of SklogWiki. If you add sufficient material to this article then please remove the {{Stub-general}} template from this page. |
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