|
|
Line 33: |
Line 33: |
| :<math>\langle \psi \rangle = \overline \psi</math> | | :<math>\langle \psi \rangle = \overline \psi</math> |
|
| |
|
| ===Entropy=== | | ===[[Entropy]]=== |
| Ref. 1 Eq. 2.70 | | Ref. 1 Eq. 2.70 |
|
| |
|
Latest revision as of 16:45, 21 November 2007
Here we have the N-particle distribution function
(Ref. 1 Eq. 2.2)
where is a normalized constant with the dimensions
of the phase space .
Normalization condition (Ref. 1 Eq. 2.3):
it is convenient to set (Ref. 1 Eq. 2.4)
where is the volume of the system and is the characteristic momentum
of the particles (Ref. 1 Eq. 3.26),
Macroscopic mean values are given by (Ref. 1 Eq. 2.5)
Ref. 1 Eq. 2.6
Ref. 1 Eq. 2.70
where is the N-particle thermal potential (Ref. 1 Eq. 2.12)
References[edit]
- G. A. Martynov "Fundamental Theory of Liquids. Method of Distribution Functions", Adam Hilger (out of print)