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Transition of ion-acoustic perturbations in multicomponent plasma with negative ions
Evolution of ion-acoustic compressive (positive) and rarefactive (negative) perturbations in a multicomponent plasma with negative ions has been investigated in a double plasma device. Transition of compressive solitons in electron-positive ion plasma, into a dispersing train of oscillations in a mu...
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Published in: | Physics of plasmas 2008-08, Vol.15 (8) |
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container_title | Physics of plasmas |
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creator | Sharma, Sumita Kumari Devi, Kavita Adhikary, Nirab Chandra Bailung, Heremba |
description | Evolution of ion-acoustic compressive (positive) and rarefactive (negative) perturbations in a multicomponent plasma with negative ions has been investigated in a double plasma device. Transition of compressive solitons in electron-positive ion plasma, into a dispersing train of oscillations in a multicomponent plasma, when the negative ion concentration
r
exceeds a critical value
r
c
, has been observed. On the other hand, an initial rarefactive perturbation initially evolves into a dispersing train of oscillations in electron-positive ion plasma and transforms into rarefactive solitons in a multicomponent plasma when the negative ion concentration is higher than the critical value. The Mach velocity and width of the compressive and rarefactive solitons are measured. The compressive solitons in the range
0
<
r
<
r
c
and the rarefactive solitons in the range
r
>
r
c
have different characteristics than the Korteweg–de Vries (KdV) solitons at
r
=
0
and modified KdV solitons at
r
=
r
c
. A nonlinear differential equation having two terms to account for the lower and higher order nonlinearity has been used to explain the observed results. |
doi_str_mv | 10.1063/1.2972164 |
format | article |
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r
exceeds a critical value
r
c
, has been observed. On the other hand, an initial rarefactive perturbation initially evolves into a dispersing train of oscillations in electron-positive ion plasma and transforms into rarefactive solitons in a multicomponent plasma when the negative ion concentration is higher than the critical value. The Mach velocity and width of the compressive and rarefactive solitons are measured. The compressive solitons in the range
0
<
r
<
r
c
and the rarefactive solitons in the range
r
>
r
c
have different characteristics than the Korteweg–de Vries (KdV) solitons at
r
=
0
and modified KdV solitons at
r
=
r
c
. A nonlinear differential equation having two terms to account for the lower and higher order nonlinearity has been used to explain the observed results.</description><identifier>ISSN: 1070-664X</identifier><identifier>EISSN: 1089-7674</identifier><identifier>DOI: 10.1063/1.2972164</identifier><identifier>CODEN: PHPAEN</identifier><language>eng</language><publisher>United States</publisher><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY ; ANIONS ; CATIONS ; ELECTRONS ; ION ACOUSTIC WAVES ; KORTEWEG-DE VRIES EQUATION ; NONLINEAR PROBLEMS ; OSCILLATIONS ; PERTURBATION THEORY ; PLASMA ; SHOCK WAVES ; SOLITONS ; VELOCITY</subject><ispartof>Physics of plasmas, 2008-08, Vol.15 (8)</ispartof><rights>American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c327t-9f8b4a78a1ae3b66f0141d096746ca87e11d372130458012c3b15c7d68941f853</citedby><cites>FETCH-LOGICAL-c327t-9f8b4a78a1ae3b66f0141d096746ca87e11d372130458012c3b15c7d68941f853</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/pop/article-lookup/doi/10.1063/1.2972164$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,776,778,780,791,881,27901,27902,76126</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/21120492$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Sharma, Sumita Kumari</creatorcontrib><creatorcontrib>Devi, Kavita</creatorcontrib><creatorcontrib>Adhikary, Nirab Chandra</creatorcontrib><creatorcontrib>Bailung, Heremba</creatorcontrib><title>Transition of ion-acoustic perturbations in multicomponent plasma with negative ions</title><title>Physics of plasmas</title><description>Evolution of ion-acoustic compressive (positive) and rarefactive (negative) perturbations in a multicomponent plasma with negative ions has been investigated in a double plasma device. Transition of compressive solitons in electron-positive ion plasma, into a dispersing train of oscillations in a multicomponent plasma, when the negative ion concentration
r
exceeds a critical value
r
c
, has been observed. On the other hand, an initial rarefactive perturbation initially evolves into a dispersing train of oscillations in electron-positive ion plasma and transforms into rarefactive solitons in a multicomponent plasma when the negative ion concentration is higher than the critical value. The Mach velocity and width of the compressive and rarefactive solitons are measured. The compressive solitons in the range
0
<
r
<
r
c
and the rarefactive solitons in the range
r
>
r
c
have different characteristics than the Korteweg–de Vries (KdV) solitons at
r
=
0
and modified KdV solitons at
r
=
r
c
. A nonlinear differential equation having two terms to account for the lower and higher order nonlinearity has been used to explain the observed results.</description><subject>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</subject><subject>ANIONS</subject><subject>CATIONS</subject><subject>ELECTRONS</subject><subject>ION ACOUSTIC WAVES</subject><subject>KORTEWEG-DE VRIES EQUATION</subject><subject>NONLINEAR PROBLEMS</subject><subject>OSCILLATIONS</subject><subject>PERTURBATION THEORY</subject><subject>PLASMA</subject><subject>SHOCK WAVES</subject><subject>SOLITONS</subject><subject>VELOCITY</subject><issn>1070-664X</issn><issn>1089-7674</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNqdkEtLxDAUhYMoOD4W_oOAK4WOuU2apEsZfMGAmxHchTRNnco0KUlmxH9v6gy4d3Uv934czjkIXQGZA-H0DuZlLUrg7AjNgMi6EFyw42kXpOCcvZ-isxg_CSGMV3KGVqugXexT7x32Hc6j0MZvY-oNHm1I29Do6Rlx7_Cw3eS7H0bvrEt43Og4aPzVpzV29iNzOzspxAt00ulNtJeHeY7eHh9Wi-di-fr0srhfFoaWIhV1JxumhdSgLW047wgwaEmdHXOjpbAALc1hKGGVJFAa2kBlRMtlzaCTFT1H13tdn_2qaPpkzdp456xJqgQoCavLTN3sKRN8jMF2agz9oMO3AqKm0hSoQ2mZvd2zk9hv8P_BOx_-QDW2Hf0BhZx6zQ</recordid><startdate>20080801</startdate><enddate>20080801</enddate><creator>Sharma, Sumita Kumari</creator><creator>Devi, Kavita</creator><creator>Adhikary, Nirab Chandra</creator><creator>Bailung, Heremba</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>20080801</creationdate><title>Transition of ion-acoustic perturbations in multicomponent plasma with negative ions</title><author>Sharma, Sumita Kumari ; Devi, Kavita ; Adhikary, Nirab Chandra ; Bailung, Heremba</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-9f8b4a78a1ae3b66f0141d096746ca87e11d372130458012c3b15c7d68941f853</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2008</creationdate><topic>70 PLASMA PHYSICS AND FUSION TECHNOLOGY</topic><topic>ANIONS</topic><topic>CATIONS</topic><topic>ELECTRONS</topic><topic>ION ACOUSTIC WAVES</topic><topic>KORTEWEG-DE VRIES EQUATION</topic><topic>NONLINEAR PROBLEMS</topic><topic>OSCILLATIONS</topic><topic>PERTURBATION THEORY</topic><topic>PLASMA</topic><topic>SHOCK WAVES</topic><topic>SOLITONS</topic><topic>VELOCITY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sharma, Sumita Kumari</creatorcontrib><creatorcontrib>Devi, Kavita</creatorcontrib><creatorcontrib>Adhikary, Nirab Chandra</creatorcontrib><creatorcontrib>Bailung, Heremba</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physics of plasmas</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sharma, Sumita Kumari</au><au>Devi, Kavita</au><au>Adhikary, Nirab Chandra</au><au>Bailung, Heremba</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transition of ion-acoustic perturbations in multicomponent plasma with negative ions</atitle><jtitle>Physics of plasmas</jtitle><date>2008-08-01</date><risdate>2008</risdate><volume>15</volume><issue>8</issue><issn>1070-664X</issn><eissn>1089-7674</eissn><coden>PHPAEN</coden><abstract>Evolution of ion-acoustic compressive (positive) and rarefactive (negative) perturbations in a multicomponent plasma with negative ions has been investigated in a double plasma device. Transition of compressive solitons in electron-positive ion plasma, into a dispersing train of oscillations in a multicomponent plasma, when the negative ion concentration
r
exceeds a critical value
r
c
, has been observed. On the other hand, an initial rarefactive perturbation initially evolves into a dispersing train of oscillations in electron-positive ion plasma and transforms into rarefactive solitons in a multicomponent plasma when the negative ion concentration is higher than the critical value. The Mach velocity and width of the compressive and rarefactive solitons are measured. The compressive solitons in the range
0
<
r
<
r
c
and the rarefactive solitons in the range
r
>
r
c
have different characteristics than the Korteweg–de Vries (KdV) solitons at
r
=
0
and modified KdV solitons at
r
=
r
c
. A nonlinear differential equation having two terms to account for the lower and higher order nonlinearity has been used to explain the observed results.</abstract><cop>United States</cop><doi>10.1063/1.2972164</doi><tpages>10</tpages></addata></record> |
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subjects | 70 PLASMA PHYSICS AND FUSION TECHNOLOGY ANIONS CATIONS ELECTRONS ION ACOUSTIC WAVES KORTEWEG-DE VRIES EQUATION NONLINEAR PROBLEMS OSCILLATIONS PERTURBATION THEORY PLASMA SHOCK WAVES SOLITONS VELOCITY |
title | Transition of ion-acoustic perturbations in multicomponent plasma with negative ions |
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