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Particle finite size effects as mean field approximation

Abstract

The equation of state for classical Boltzmann gas with two-particle interaction can be written off any approximations in single-particle representation and/or in terms of the phenomenological mean field model. Using the latter it is suggested to take into account the finite size of particles of the medium in a thermodynamically consistent way. The possible arising of the intermediate statistics is pointed out. 15 refs.; 1 fig. (author).
Authors:
Publication Date:
Dec 31, 1991
Product Type:
Technical Report
Report Number:
ITP-91-40
Reference Number:
SCA: 663110; PA: AIX-24:028213; SN: 93000951514
Resource Relation:
Other Information: PBD: 1991
Subject:
73 NUCLEAR PHYSICS AND RADIATION PHYSICS; BOLTZMANN STATISTICS; HARD-CORE POTENTIAL; MEAN-FIELD THEORY; EQUATIONS OF STATE; INTERACTION RANGE; SINGLE-PARTICLE MODEL; THERMODYNAMIC MODEL; 663110; GENERAL AND AVERAGE PROPERTIES OF NUCLEI AND NUCLEAR ENERGY LEVELS
OSTI ID:
10129615
Research Organizations:
AN Ukrainskoj SSR, Kiev (Ukraine). Inst. Teoreticheskoj Fiziki
Country of Origin:
Ukraine
Language:
English
Other Identifying Numbers:
Other: ON: DE93618705; TRN: UA9300002028213
Availability:
OSTI; NTIS (US Sales Only); INIS
Submitting Site:
INIS
Size:
[16] p.
Announcement Date:
Jul 04, 2005

Citation Formats

Anchishkin, D. Particle finite size effects as mean field approximation. Ukraine: N. p., 1991. Web.
Anchishkin, D. Particle finite size effects as mean field approximation. Ukraine.
Anchishkin, D. 1991. "Particle finite size effects as mean field approximation." Ukraine.
@misc{etde_10129615,
title = {Particle finite size effects as mean field approximation}
author = {Anchishkin, D}
abstractNote = {The equation of state for classical Boltzmann gas with two-particle interaction can be written off any approximations in single-particle representation and/or in terms of the phenomenological mean field model. Using the latter it is suggested to take into account the finite size of particles of the medium in a thermodynamically consistent way. The possible arising of the intermediate statistics is pointed out. 15 refs.; 1 fig. (author).}
place = {Ukraine}
year = {1991}
month = {Dec}
}