The excitation of an independent-particle gas by a time dependent potential well

The order-to-chaos transition in the dynamics of independent classical particles gas was studied by means of the numerical simulations. The excitation of the gas for containers whose surfaces are rippled according to Legendre polynomials P2 , P3, P4 , P5 , P6 was followed for ten periods of oscillat...

Full description

Bibliographic Details
Main Authors: J. P. Błocki, A. G. Magner, I. S. Yatsyshyn
Format: Article
Language:English
Published: Institute for Nuclear Research, National Academy of Sciences of Ukraine 2010-09-01
Series:Âderna Fìzika ta Energetika
Subjects:
Online Access:http://jnpae.kinr.kiev.ua/11.3/Articles_PDF/jnpae-2010-11-0239-Blocki.pdf
id doaj-415a72dbb7344dfcaf44ec9cd271308f
record_format Article
spelling doaj-415a72dbb7344dfcaf44ec9cd271308f2020-11-24T23:40:20ZengInstitute for Nuclear Research, National Academy of Sciences of UkraineÂderna Fìzika ta Energetika1818-331X2074-05652010-09-01113239245The excitation of an independent-particle gas by a time dependent potential wellJ. P. Błocki0A. G. Magner1I. S. Yatsyshyn2A. Soltan Institute for Nuclear Studies, Swierk/Otwock, Polandnstitute for Nuclear Research, National Academy of Sciences of Ukraine, Kyiv, Ukrainenstitute for Nuclear Research, National Academy of Sciences of Ukraine, Kyiv, UkraineThe order-to-chaos transition in the dynamics of independent classical particles gas was studied by means of the numerical simulations. The excitation of the gas for containers whose surfaces are rippled according to Legendre polynomials P2 , P3, P4 , P5 , P6 was followed for ten periods of oscillations. Spheroidal deformations were also considered. Poincare sections and Lyapunov exponents have been calculated showing different degrees of chaoticity depending on the shape and amplitude of oscillations. For 2 P polynomial the reaction of a gas to the periodic container deformation is mostly elastic as 2 P deformation especially for not very big deformations is almost like an integrable spheroid. For other polynomials the situation is more or less chaotic with a chaoticity increasing with the increasing order of the polynomial.http://jnpae.kinr.kiev.ua/11.3/Articles_PDF/jnpae-2010-11-0239-Blocki.pdfone-body dissipationorder-to-chaos transitionsnuclear collective dynamics
collection DOAJ
language English
format Article
sources DOAJ
author J. P. Błocki
A. G. Magner
I. S. Yatsyshyn
spellingShingle J. P. Błocki
A. G. Magner
I. S. Yatsyshyn
The excitation of an independent-particle gas by a time dependent potential well
Âderna Fìzika ta Energetika
one-body dissipation
order-to-chaos transitions
nuclear collective dynamics
author_facet J. P. Błocki
A. G. Magner
I. S. Yatsyshyn
author_sort J. P. Błocki
title The excitation of an independent-particle gas by a time dependent potential well
title_short The excitation of an independent-particle gas by a time dependent potential well
title_full The excitation of an independent-particle gas by a time dependent potential well
title_fullStr The excitation of an independent-particle gas by a time dependent potential well
title_full_unstemmed The excitation of an independent-particle gas by a time dependent potential well
title_sort excitation of an independent-particle gas by a time dependent potential well
publisher Institute for Nuclear Research, National Academy of Sciences of Ukraine
series Âderna Fìzika ta Energetika
issn 1818-331X
2074-0565
publishDate 2010-09-01
description The order-to-chaos transition in the dynamics of independent classical particles gas was studied by means of the numerical simulations. The excitation of the gas for containers whose surfaces are rippled according to Legendre polynomials P2 , P3, P4 , P5 , P6 was followed for ten periods of oscillations. Spheroidal deformations were also considered. Poincare sections and Lyapunov exponents have been calculated showing different degrees of chaoticity depending on the shape and amplitude of oscillations. For 2 P polynomial the reaction of a gas to the periodic container deformation is mostly elastic as 2 P deformation especially for not very big deformations is almost like an integrable spheroid. For other polynomials the situation is more or less chaotic with a chaoticity increasing with the increasing order of the polynomial.
topic one-body dissipation
order-to-chaos transitions
nuclear collective dynamics
url http://jnpae.kinr.kiev.ua/11.3/Articles_PDF/jnpae-2010-11-0239-Blocki.pdf
work_keys_str_mv AT jpbłocki theexcitationofanindependentparticlegasbyatimedependentpotentialwell
AT agmagner theexcitationofanindependentparticlegasbyatimedependentpotentialwell
AT isyatsyshyn theexcitationofanindependentparticlegasbyatimedependentpotentialwell
AT jpbłocki excitationofanindependentparticlegasbyatimedependentpotentialwell
AT agmagner excitationofanindependentparticlegasbyatimedependentpotentialwell
AT isyatsyshyn excitationofanindependentparticlegasbyatimedependentpotentialwell
_version_ 1725510062061912064