BBGKY hierarchy: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) No edit summary |
Carl McBride (talk | contribs) No edit summary |
||
| Line 1: | Line 1: | ||
{{Stub-general}} | |||
The '''BBGKY hierarchy''' consists of distribution functions, named after Bogolyubov, Born, Green, [[John G. Kirkwood | Kirkwood]] and Yvon. | The '''BBGKY hierarchy''' consists of distribution functions, named after Bogolyubov, Born, Green, [[John G. Kirkwood | Kirkwood]] and Yvon. | ||
The BBGKY hierarchy is a system of equations for the dynamical behavior of fluids, | The BBGKY hierarchy is a system of equations for the dynamical behavior of fluids, | ||
Revision as of 15:00, 27 September 2007
|
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. |
The BBGKY hierarchy consists of distribution functions, named after Bogolyubov, Born, Green, Kirkwood and Yvon. The BBGKY hierarchy is a system of equations for the dynamical behavior of fluids, with the important extension to dense liquids. The equations are exact, and relate the phase space probability density for n+1 particles to the phase space probability density for n particles . In Ref. 1 it is shown that the H-theorem follows from the Kirkwood superposition approximation.