Stochastic perturbation and relaxation of a classical Coulomb plasma
Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Tkachev, A. N. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1997 |
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| Schlagwörter: |
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| Anmerkung: |
© American Institute of Physics 1997 |
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| Übergeordnetes Werk: |
Enthalten in: Technical physics letters - Nauka/Interperiodica, 1993, 23(1997), 9 vom: Sept., Seite 686-689 |
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| Übergeordnetes Werk: |
volume:23 ; year:1997 ; number:9 ; month:09 ; pages:686-689 |
| Links: |
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| DOI / URN: |
10.1134/1.1261656 |
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| Katalog-ID: |
OLC2072842557 |
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| 520 | |a Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. | ||
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10.1134/1.1261656 doi (DE-627)OLC2072842557 (DE-He213)1.1261656-p DE-627 ger DE-627 rakwb eng 530 VZ Tkachev, A. N. verfasserin aut Stochastic perturbation and relaxation of a classical Coulomb plasma 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © American Institute of Physics 1997 Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. Recombination Kinetic Equation Dynamical Equation Particle Velocity Kinetic Theory Yakovlenko, S. I. aut Enthalten in Technical physics letters Nauka/Interperiodica, 1993 23(1997), 9 vom: Sept., Seite 686-689 (DE-627)171149521 (DE-600)1158056-2 (DE-576)038488426 1063-7850 nnns volume:23 year:1997 number:9 month:09 pages:686-689 https://doi.org/10.1134/1.1261656 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2014 GBV_ILN_2016 GBV_ILN_4700 AR 23 1997 9 09 686-689 |
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10.1134/1.1261656 doi (DE-627)OLC2072842557 (DE-He213)1.1261656-p DE-627 ger DE-627 rakwb eng 530 VZ Tkachev, A. N. verfasserin aut Stochastic perturbation and relaxation of a classical Coulomb plasma 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © American Institute of Physics 1997 Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. Recombination Kinetic Equation Dynamical Equation Particle Velocity Kinetic Theory Yakovlenko, S. I. aut Enthalten in Technical physics letters Nauka/Interperiodica, 1993 23(1997), 9 vom: Sept., Seite 686-689 (DE-627)171149521 (DE-600)1158056-2 (DE-576)038488426 1063-7850 nnns volume:23 year:1997 number:9 month:09 pages:686-689 https://doi.org/10.1134/1.1261656 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2014 GBV_ILN_2016 GBV_ILN_4700 AR 23 1997 9 09 686-689 |
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10.1134/1.1261656 doi (DE-627)OLC2072842557 (DE-He213)1.1261656-p DE-627 ger DE-627 rakwb eng 530 VZ Tkachev, A. N. verfasserin aut Stochastic perturbation and relaxation of a classical Coulomb plasma 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © American Institute of Physics 1997 Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. Recombination Kinetic Equation Dynamical Equation Particle Velocity Kinetic Theory Yakovlenko, S. I. aut Enthalten in Technical physics letters Nauka/Interperiodica, 1993 23(1997), 9 vom: Sept., Seite 686-689 (DE-627)171149521 (DE-600)1158056-2 (DE-576)038488426 1063-7850 nnns volume:23 year:1997 number:9 month:09 pages:686-689 https://doi.org/10.1134/1.1261656 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2014 GBV_ILN_2016 GBV_ILN_4700 AR 23 1997 9 09 686-689 |
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10.1134/1.1261656 doi (DE-627)OLC2072842557 (DE-He213)1.1261656-p DE-627 ger DE-627 rakwb eng 530 VZ Tkachev, A. N. verfasserin aut Stochastic perturbation and relaxation of a classical Coulomb plasma 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © American Institute of Physics 1997 Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. Recombination Kinetic Equation Dynamical Equation Particle Velocity Kinetic Theory Yakovlenko, S. I. aut Enthalten in Technical physics letters Nauka/Interperiodica, 1993 23(1997), 9 vom: Sept., Seite 686-689 (DE-627)171149521 (DE-600)1158056-2 (DE-576)038488426 1063-7850 nnns volume:23 year:1997 number:9 month:09 pages:686-689 https://doi.org/10.1134/1.1261656 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2014 GBV_ILN_2016 GBV_ILN_4700 AR 23 1997 9 09 686-689 |
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Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. © American Institute of Physics 1997 |
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Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. © American Institute of Physics 1997 |
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Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory. © American Institute of Physics 1997 |
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N.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Stochastic perturbation and relaxation of a classical Coulomb plasma</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1997</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© American Institute of Physics 1997</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract It is shown that the dynamic mixing of phase trajectories in a system of classical Coulomb particles does not result in the recombination described by the kinetic equations. The effect of the imprecision of the computational method and the effect of permutation of the particle velocities on recombination relaxation is studied. The imprecision of the numerical integration of the dynamical equations results in a loss of reversibility of the solution and in anomalously slow (in exact calculations) relaxation. If the permutations of the particle velocities are made with a rate higher than the rate of Coulomb collisions, recombination relaxation proceeds in accordance with kinetic theory.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Recombination</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Kinetic Equation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Dynamical Equation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Particle Velocity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Kinetic Theory</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yakovlenko, S. I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Technical physics letters</subfield><subfield code="d">Nauka/Interperiodica, 1993</subfield><subfield code="g">23(1997), 9 vom: Sept., Seite 686-689</subfield><subfield code="w">(DE-627)171149521</subfield><subfield code="w">(DE-600)1158056-2</subfield><subfield code="w">(DE-576)038488426</subfield><subfield code="x">1063-7850</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:23</subfield><subfield code="g">year:1997</subfield><subfield code="g">number:9</subfield><subfield code="g">month:09</subfield><subfield code="g">pages:686-689</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.1261656</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_130</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2016</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">23</subfield><subfield code="j">1997</subfield><subfield code="e">9</subfield><subfield code="c">09</subfield><subfield code="h">686-689</subfield></datafield></record></collection>
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