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Magnetic field amplification and saturation in turbulence behind a relativistic shock
We have investigated via 2D relativistic magnetohydrodynamic simulations the long-term evolution of turbulence created by a relativistic shock propagating through an inhomogeneous medium. In the post-shock region, magnetic field is strongly amplified by turbulent motions triggered by pre-shock densi...
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Published in: | Monthly notices of the Royal Astronomical Society 2014-04, Vol.439 (4), p.3490-3503 |
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container_title | Monthly notices of the Royal Astronomical Society |
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creator | Mizuno, Yosuke Pohl, Martin Niemiec, Jacek Zhang, Bing Nishikawa, Ken-Ichi Hardee, Philip E. |
description | We have investigated via 2D relativistic magnetohydrodynamic simulations the long-term evolution of turbulence created by a relativistic shock propagating through an inhomogeneous medium. In the post-shock region, magnetic field is strongly amplified by turbulent motions triggered by pre-shock density inhomogeneities. Using a long-simulation box we have followed the magnetic field amplification until it is fully developed and saturated. The turbulent velocity is subrelativistic even for a strong shock. Magnetic field amplification is controlled by the turbulent motion and saturation occurs when the magnetic energy is comparable to the turbulent kinetic energy. Magnetic field amplification and saturation depend on the initial strength and direction of the magnetic field in the pre-shock medium, and on the shock strength. If the initial magnetic field is perpendicular to the shock normal, the magnetic field is first compressed at the shock and then can be amplified by turbulent motion in the post-shock region. Saturation occurs when the magnetic energy becomes comparable to the turbulent kinetic energy in the post-shock region. If the initial magnetic field in the pre-shock medium is strong, the post-shock region becomes turbulent but significant field amplification does not occur. If the magnetic energy after shock compression is larger than the turbulent kinetic energy in the post-shock region, significant field amplification does not occur. We discuss possible applications of our results to gamma-ray bursts and active galactic nuclei. |
doi_str_mv | 10.1093/mnras/stu196 |
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In the post-shock region, magnetic field is strongly amplified by turbulent motions triggered by pre-shock density inhomogeneities. Using a long-simulation box we have followed the magnetic field amplification until it is fully developed and saturated. The turbulent velocity is subrelativistic even for a strong shock. Magnetic field amplification is controlled by the turbulent motion and saturation occurs when the magnetic energy is comparable to the turbulent kinetic energy. Magnetic field amplification and saturation depend on the initial strength and direction of the magnetic field in the pre-shock medium, and on the shock strength. If the initial magnetic field is perpendicular to the shock normal, the magnetic field is first compressed at the shock and then can be amplified by turbulent motion in the post-shock region. Saturation occurs when the magnetic energy becomes comparable to the turbulent kinetic energy in the post-shock region. If the initial magnetic field in the pre-shock medium is strong, the post-shock region becomes turbulent but significant field amplification does not occur. If the magnetic energy after shock compression is larger than the turbulent kinetic energy in the post-shock region, significant field amplification does not occur. We discuss possible applications of our results to gamma-ray bursts and active galactic nuclei.</description><identifier>ISSN: 0035-8711</identifier><identifier>EISSN: 1365-2966</identifier><identifier>DOI: 10.1093/mnras/stu196</identifier><language>eng</language><publisher>London: Oxford University Press</publisher><subject>Fluid mechanics ; Gamma ray astronomy ; Magnetic fields ; Simulation ; Starbursts ; Turbulence</subject><ispartof>Monthly notices of the Royal Astronomical Society, 2014-04, Vol.439 (4), p.3490-3503</ispartof><rights>2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society 2014</rights><rights>Copyright Oxford University Press, UK Apr 21, 2014</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c399t-8da39a2c7036af6d83834dda8305d7079313c15025703900b685765dcc8900603</citedby><cites>FETCH-LOGICAL-c399t-8da39a2c7036af6d83834dda8305d7079313c15025703900b685765dcc8900603</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,1598,27901,27902</link.rule.ids><linktorsrc>$$Uhttps://dx.doi.org/10.1093/mnras/stu196$$EView_record_in_Oxford_University_Press$$FView_record_in_$$GOxford_University_Press</linktorsrc></links><search><creatorcontrib>Mizuno, Yosuke</creatorcontrib><creatorcontrib>Pohl, Martin</creatorcontrib><creatorcontrib>Niemiec, Jacek</creatorcontrib><creatorcontrib>Zhang, Bing</creatorcontrib><creatorcontrib>Nishikawa, Ken-Ichi</creatorcontrib><creatorcontrib>Hardee, Philip E.</creatorcontrib><title>Magnetic field amplification and saturation in turbulence behind a relativistic shock</title><title>Monthly notices of the Royal Astronomical Society</title><addtitle>Mon. Not. R. Astron. Soc</addtitle><description>We have investigated via 2D relativistic magnetohydrodynamic simulations the long-term evolution of turbulence created by a relativistic shock propagating through an inhomogeneous medium. In the post-shock region, magnetic field is strongly amplified by turbulent motions triggered by pre-shock density inhomogeneities. Using a long-simulation box we have followed the magnetic field amplification until it is fully developed and saturated. The turbulent velocity is subrelativistic even for a strong shock. Magnetic field amplification is controlled by the turbulent motion and saturation occurs when the magnetic energy is comparable to the turbulent kinetic energy. Magnetic field amplification and saturation depend on the initial strength and direction of the magnetic field in the pre-shock medium, and on the shock strength. If the initial magnetic field is perpendicular to the shock normal, the magnetic field is first compressed at the shock and then can be amplified by turbulent motion in the post-shock region. Saturation occurs when the magnetic energy becomes comparable to the turbulent kinetic energy in the post-shock region. If the initial magnetic field in the pre-shock medium is strong, the post-shock region becomes turbulent but significant field amplification does not occur. If the magnetic energy after shock compression is larger than the turbulent kinetic energy in the post-shock region, significant field amplification does not occur. We discuss possible applications of our results to gamma-ray bursts and active galactic nuclei.</description><subject>Fluid mechanics</subject><subject>Gamma ray astronomy</subject><subject>Magnetic fields</subject><subject>Simulation</subject><subject>Starbursts</subject><subject>Turbulence</subject><issn>0035-8711</issn><issn>1365-2966</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp9kD9PwzAUxC0EEqWw8QEsMbAQ-hzXjj2iin9SEQudLcd2qEvqBDtB4tvjEmamd6f76Z50CF0SuCUg6WIfok6LNIxE8iM0I5SzopScH6MZAGWFqAg5RWcp7QBgSUs-Q5sX_R7c4A1uvGst1vu-9Y03evBdwDpYnPQwxsn6gLOux9YF43Dttj7nGkfX5vzLp0NN2nbm4xydNLpN7uLvztHm4f5t9VSsXx-fV3frwlAph0JYTaUuTQWU64ZbQQVdWqsFBWYrqCQl1BAGJcuEBKi5YBVn1hiRHQc6R1dTbx-7z9GlQe26MYb8UhFGiCRLkCxTNxNlYpdSdI3qo9_r-K0IqMNw6nc4NQ2X8esJ78b-f_IHZtVv9g</recordid><startdate>20140421</startdate><enddate>20140421</enddate><creator>Mizuno, Yosuke</creator><creator>Pohl, Martin</creator><creator>Niemiec, Jacek</creator><creator>Zhang, Bing</creator><creator>Nishikawa, Ken-Ichi</creator><creator>Hardee, Philip E.</creator><general>Oxford University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20140421</creationdate><title>Magnetic field amplification and saturation in turbulence behind a relativistic shock</title><author>Mizuno, Yosuke ; Pohl, Martin ; Niemiec, Jacek ; Zhang, Bing ; Nishikawa, Ken-Ichi ; Hardee, Philip E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c399t-8da39a2c7036af6d83834dda8305d7079313c15025703900b685765dcc8900603</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Fluid mechanics</topic><topic>Gamma ray astronomy</topic><topic>Magnetic fields</topic><topic>Simulation</topic><topic>Starbursts</topic><topic>Turbulence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mizuno, Yosuke</creatorcontrib><creatorcontrib>Pohl, Martin</creatorcontrib><creatorcontrib>Niemiec, Jacek</creatorcontrib><creatorcontrib>Zhang, Bing</creatorcontrib><creatorcontrib>Nishikawa, Ken-Ichi</creatorcontrib><creatorcontrib>Hardee, Philip E.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Monthly notices of the Royal Astronomical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Mizuno, Yosuke</au><au>Pohl, Martin</au><au>Niemiec, Jacek</au><au>Zhang, Bing</au><au>Nishikawa, Ken-Ichi</au><au>Hardee, Philip E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetic field amplification and saturation in turbulence behind a relativistic shock</atitle><jtitle>Monthly notices of the Royal Astronomical Society</jtitle><stitle>Mon. Not. R. Astron. Soc</stitle><date>2014-04-21</date><risdate>2014</risdate><volume>439</volume><issue>4</issue><spage>3490</spage><epage>3503</epage><pages>3490-3503</pages><issn>0035-8711</issn><eissn>1365-2966</eissn><abstract>We have investigated via 2D relativistic magnetohydrodynamic simulations the long-term evolution of turbulence created by a relativistic shock propagating through an inhomogeneous medium. In the post-shock region, magnetic field is strongly amplified by turbulent motions triggered by pre-shock density inhomogeneities. Using a long-simulation box we have followed the magnetic field amplification until it is fully developed and saturated. The turbulent velocity is subrelativistic even for a strong shock. Magnetic field amplification is controlled by the turbulent motion and saturation occurs when the magnetic energy is comparable to the turbulent kinetic energy. Magnetic field amplification and saturation depend on the initial strength and direction of the magnetic field in the pre-shock medium, and on the shock strength. If the initial magnetic field is perpendicular to the shock normal, the magnetic field is first compressed at the shock and then can be amplified by turbulent motion in the post-shock region. Saturation occurs when the magnetic energy becomes comparable to the turbulent kinetic energy in the post-shock region. If the initial magnetic field in the pre-shock medium is strong, the post-shock region becomes turbulent but significant field amplification does not occur. If the magnetic energy after shock compression is larger than the turbulent kinetic energy in the post-shock region, significant field amplification does not occur. 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subjects | Fluid mechanics Gamma ray astronomy Magnetic fields Simulation Starbursts Turbulence |
title | Magnetic field amplification and saturation in turbulence behind a relativistic shock |
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