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Self-similar evolution of the two-dimensional cylindrical magnetohydrodynamic flux rope
One of the important features of the one-dimensional cylindrical self-similar magnetohydrodynamic (MHD) model of magnetic rope is that it oscillates about a force-free solution [Osherovich et al., 1993. Nonlinear evolution of magnetic flux ropes. 1. Low-beta limit. Journal of Geophysical Research 98...
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Published in: | Journal of atmospheric and solar-terrestrial physics 2005-12, Vol.67 (17), p.1691-1696 |
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description | One of the important features of the one-dimensional cylindrical self-similar magnetohydrodynamic (MHD) model of magnetic rope is that it oscillates about a force-free solution [Osherovich et al., 1993. Nonlinear evolution of magnetic flux ropes. 1. Low-beta limit. Journal of Geophysical Research 98, 13225–13231; Osherovich et al., 1995. Nonlinear evolution of magnetic flux ropes. 2. Finite-beta plasma. Journal of Geophysical Research 100, 12307-12318.] due to the reduced dimensionality of the system, as in laboratory Z pinch plasmas [Felber, 1982. Self-similar oscillations of a Z pinch. Physics of Fluids 25, 643–645]. However, such oscillations have never been confirmed by observations. Following the approach of Low [1982a. Self-similar magnetohydrodynamics. I. The
γ
=
4
/
3
Polytrope and the Coronal transient. Astrophysical Journal 254, 796–805; 1982b. Self-similar magnetohydrodynamics. II. The expansion of a Stella envelope into a surrounding vacuum. Astrophysical Journal 261, 351–369], a two-dimensional self-similar MHD model under radial expansion is analyzed in cylindrical geometry with translational symmetry in the
z-axis. Non-oscillatory solutions are established with polytropic index
γ
=
1
and 2. For
γ
=
2
, the system is linear, and the plasma pressure is balanced by the longitudinal magnetic pressure. As for
γ
=
1
, the plasma pressure is balanced by the transverse magnetic pressure, and it is also the driving force of non-linearity that stresses the system. Due to the two-dimensional structure of the magnetic field and plasma, this model allows the possibility of an energetic magnetic cloud with a southward component impinging on Earth without raising expected magnetic storms. |
doi_str_mv | 10.1016/j.jastp.2004.11.011 |
format | article |
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γ
=
4
/
3
Polytrope and the Coronal transient. Astrophysical Journal 254, 796–805; 1982b. Self-similar magnetohydrodynamics. II. The expansion of a Stella envelope into a surrounding vacuum. Astrophysical Journal 261, 351–369], a two-dimensional self-similar MHD model under radial expansion is analyzed in cylindrical geometry with translational symmetry in the
z-axis. Non-oscillatory solutions are established with polytropic index
γ
=
1
and 2. For
γ
=
2
, the system is linear, and the plasma pressure is balanced by the longitudinal magnetic pressure. As for
γ
=
1
, the plasma pressure is balanced by the transverse magnetic pressure, and it is also the driving force of non-linearity that stresses the system. Due to the two-dimensional structure of the magnetic field and plasma, this model allows the possibility of an energetic magnetic cloud with a southward component impinging on Earth without raising expected magnetic storms.</description><identifier>ISSN: 1364-6826</identifier><identifier>EISSN: 1879-1824</identifier><identifier>DOI: 10.1016/j.jastp.2004.11.011</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Earth, ocean, space ; Exact sciences and technology ; External geophysics ; Magnetic rope ; Physics of the high neutral atmosphere ; Physics of the ionosphere ; Physics of the magnetosphere ; Self-similar MHD</subject><ispartof>Journal of atmospheric and solar-terrestrial physics, 2005-12, Vol.67 (17), p.1691-1696</ispartof><rights>2005 Elsevier Ltd</rights><rights>2006 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c426t-70993a0f1586e3259523491ca4889c386653ab1c4223e1838084a094c3132fb53</citedby><cites>FETCH-LOGICAL-c426t-70993a0f1586e3259523491ca4889c386653ab1c4223e1838084a094c3132fb53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,776,780,785,786,23909,23910,25118,27901,27902</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=17446885$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Tsui, K.H.</creatorcontrib><creatorcontrib>Tavares, M.D.</creatorcontrib><title>Self-similar evolution of the two-dimensional cylindrical magnetohydrodynamic flux rope</title><title>Journal of atmospheric and solar-terrestrial physics</title><description>One of the important features of the one-dimensional cylindrical self-similar magnetohydrodynamic (MHD) model of magnetic rope is that it oscillates about a force-free solution [Osherovich et al., 1993. Nonlinear evolution of magnetic flux ropes. 1. Low-beta limit. Journal of Geophysical Research 98, 13225–13231; Osherovich et al., 1995. Nonlinear evolution of magnetic flux ropes. 2. Finite-beta plasma. Journal of Geophysical Research 100, 12307-12318.] due to the reduced dimensionality of the system, as in laboratory Z pinch plasmas [Felber, 1982. Self-similar oscillations of a Z pinch. Physics of Fluids 25, 643–645]. However, such oscillations have never been confirmed by observations. Following the approach of Low [1982a. Self-similar magnetohydrodynamics. I. The
γ
=
4
/
3
Polytrope and the Coronal transient. Astrophysical Journal 254, 796–805; 1982b. Self-similar magnetohydrodynamics. II. The expansion of a Stella envelope into a surrounding vacuum. Astrophysical Journal 261, 351–369], a two-dimensional self-similar MHD model under radial expansion is analyzed in cylindrical geometry with translational symmetry in the
z-axis. Non-oscillatory solutions are established with polytropic index
γ
=
1
and 2. For
γ
=
2
, the system is linear, and the plasma pressure is balanced by the longitudinal magnetic pressure. As for
γ
=
1
, the plasma pressure is balanced by the transverse magnetic pressure, and it is also the driving force of non-linearity that stresses the system. Due to the two-dimensional structure of the magnetic field and plasma, this model allows the possibility of an energetic magnetic cloud with a southward component impinging on Earth without raising expected magnetic storms.</description><subject>Earth, ocean, space</subject><subject>Exact sciences and technology</subject><subject>External geophysics</subject><subject>Magnetic rope</subject><subject>Physics of the high neutral atmosphere</subject><subject>Physics of the ionosphere</subject><subject>Physics of the magnetosphere</subject><subject>Self-similar MHD</subject><issn>1364-6826</issn><issn>1879-1824</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNqFkU1LxDAQhoso-PkLvPSit9ZMkqbJwYOIXyB4UPEYYjrVLGmzJl11_71ZV_Cmp3kZnnmHmbcoDoHUQECczOqZSdO8poTwGqAmABvFDshWVSAp38yaCV4JScV2sZvSjBDSUil2iqd79H2V3OC8iSW-B7-YXBjL0JfTK5bTR6g6N-CYctP40i69G7vobNaDeRlxCq_LLoZuOZrB2bL3i88yhjnuF1u98QkPfupe8Xh58XB-Xd3eXd2cn91WllMxVS1RihnSQyMFMtqohjKuwBoupbJMCtEw8wwZpgxBMkkkN0Rxy4DR_rlhe8Xx2ncew9sC06QHlyx6b0YMi6SpIqwljP0PSsi-gv8LQguKAlk5sjVoY0gpYq_n0Q0mLjUQvYpFz_R3LHoViwbQOZY8dfRjb1L-Yh_NaF36HW05F1KuDjtdc5i_9-4w6mQdjhY7F9FOugvuzz1f2jyjWA</recordid><startdate>20051201</startdate><enddate>20051201</enddate><creator>Tsui, K.H.</creator><creator>Tavares, M.D.</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>KL.</scope><scope>8FD</scope><scope>FR3</scope><scope>KR7</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20051201</creationdate><title>Self-similar evolution of the two-dimensional cylindrical magnetohydrodynamic flux rope</title><author>Tsui, K.H. ; Tavares, M.D.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c426t-70993a0f1586e3259523491ca4889c386653ab1c4223e1838084a094c3132fb53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><topic>Earth, ocean, space</topic><topic>Exact sciences and technology</topic><topic>External geophysics</topic><topic>Magnetic rope</topic><topic>Physics of the high neutral atmosphere</topic><topic>Physics of the ionosphere</topic><topic>Physics of the magnetosphere</topic><topic>Self-similar MHD</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tsui, K.H.</creatorcontrib><creatorcontrib>Tavares, M.D.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of atmospheric and solar-terrestrial physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tsui, K.H.</au><au>Tavares, M.D.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Self-similar evolution of the two-dimensional cylindrical magnetohydrodynamic flux rope</atitle><jtitle>Journal of atmospheric and solar-terrestrial physics</jtitle><date>2005-12-01</date><risdate>2005</risdate><volume>67</volume><issue>17</issue><spage>1691</spage><epage>1696</epage><pages>1691-1696</pages><issn>1364-6826</issn><eissn>1879-1824</eissn><abstract>One of the important features of the one-dimensional cylindrical self-similar magnetohydrodynamic (MHD) model of magnetic rope is that it oscillates about a force-free solution [Osherovich et al., 1993. Nonlinear evolution of magnetic flux ropes. 1. Low-beta limit. Journal of Geophysical Research 98, 13225–13231; Osherovich et al., 1995. Nonlinear evolution of magnetic flux ropes. 2. Finite-beta plasma. Journal of Geophysical Research 100, 12307-12318.] due to the reduced dimensionality of the system, as in laboratory Z pinch plasmas [Felber, 1982. Self-similar oscillations of a Z pinch. Physics of Fluids 25, 643–645]. However, such oscillations have never been confirmed by observations. Following the approach of Low [1982a. Self-similar magnetohydrodynamics. I. The
γ
=
4
/
3
Polytrope and the Coronal transient. Astrophysical Journal 254, 796–805; 1982b. Self-similar magnetohydrodynamics. II. The expansion of a Stella envelope into a surrounding vacuum. Astrophysical Journal 261, 351–369], a two-dimensional self-similar MHD model under radial expansion is analyzed in cylindrical geometry with translational symmetry in the
z-axis. Non-oscillatory solutions are established with polytropic index
γ
=
1
and 2. For
γ
=
2
, the system is linear, and the plasma pressure is balanced by the longitudinal magnetic pressure. As for
γ
=
1
, the plasma pressure is balanced by the transverse magnetic pressure, and it is also the driving force of non-linearity that stresses the system. Due to the two-dimensional structure of the magnetic field and plasma, this model allows the possibility of an energetic magnetic cloud with a southward component impinging on Earth without raising expected magnetic storms.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.jastp.2004.11.011</doi><tpages>6</tpages></addata></record> |
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subjects | Earth, ocean, space Exact sciences and technology External geophysics Magnetic rope Physics of the high neutral atmosphere Physics of the ionosphere Physics of the magnetosphere Self-similar MHD |
title | Self-similar evolution of the two-dimensional cylindrical magnetohydrodynamic flux rope |
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