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Whistler mode waves for ring distribution with A.C. electric field in inner magnetosphere of Saturn
Whistler mode waves can propagate upstream without collision impact. They are generated in these areas of vibration. They are known to play a crucial role in thermodynamics and electron acceleration. Sometimes, in some cases, they are seen as waves that strike the wavefront. Mercury, Earth, Venus an...
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Published in: | Astrophysics and space science 2018-12, Vol.363 (12), p.1, Article 249 |
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description | Whistler mode waves can propagate upstream without collision impact. They are generated in these areas of vibration. They are known to play a crucial role in thermodynamics and electron acceleration. Sometimes, in some cases, they are seen as waves that strike the wavefront. Mercury, Earth, Venus and Saturn are the planets where whistlers have been recorded in the upstream regions. They are right handed waves and can be left-hand polarized in the frame of spacecraft due to the strong negative Doppler shift. The weaker Doppler shift owes to the large angle between magnetic field vectors at 10 AU (Astronomical unit) and the solar wind velocity. These waves propagate with an angle between 10 to 60 degrees to background magnetic field. In the present paper, we took an advantage of Cassini present in the Saturnian magnetosphere to explore the whistler mode wave’s importance. A dispersion relation for obliquely as well as for whistler waves propagating perpendicular to the magnetic field, has been applied to Saturnian magnetosphere. Using the observations made by Voyager and Cassini, growth rate has been determined for non-relativistic plasma. Whistler waves are excited by temperature anisotropy, where the vertical temperature is higher than the parallel temperature. The effect of electron density, temperature anisotropy, energy density with some other parameters on the growth of whistler mode emission is studied. The result is found to be in good agreement with observations. Whistler mode wave interaction with particles basically emphasizes on the increase (decrease) in the energy of resonant particles and this variation is related to the transfer of energy to (from) other resonant particle group where the wave is the mediator of the energization process. Due to the non-monotonic nature of the ring distribution, at vertical velocities, the magnification produced by this instability is larger than the typical bi-Maxwellian anisotropy distribution because the wave can maintain resonance over a longer portion of its orbit. |
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S.</creator><creatorcontrib>Kumari, Jyoti ; Pandey, R. S.</creatorcontrib><description>Whistler mode waves can propagate upstream without collision impact. They are generated in these areas of vibration. They are known to play a crucial role in thermodynamics and electron acceleration. Sometimes, in some cases, they are seen as waves that strike the wavefront. Mercury, Earth, Venus and Saturn are the planets where whistlers have been recorded in the upstream regions. They are right handed waves and can be left-hand polarized in the frame of spacecraft due to the strong negative Doppler shift. The weaker Doppler shift owes to the large angle between magnetic field vectors at 10 AU (Astronomical unit) and the solar wind velocity. These waves propagate with an angle between 10 to 60 degrees to background magnetic field. In the present paper, we took an advantage of Cassini present in the Saturnian magnetosphere to explore the whistler mode wave’s importance. A dispersion relation for obliquely as well as for whistler waves propagating perpendicular to the magnetic field, has been applied to Saturnian magnetosphere. Using the observations made by Voyager and Cassini, growth rate has been determined for non-relativistic plasma. Whistler waves are excited by temperature anisotropy, where the vertical temperature is higher than the parallel temperature. The effect of electron density, temperature anisotropy, energy density with some other parameters on the growth of whistler mode emission is studied. The result is found to be in good agreement with observations. Whistler mode wave interaction with particles basically emphasizes on the increase (decrease) in the energy of resonant particles and this variation is related to the transfer of energy to (from) other resonant particle group where the wave is the mediator of the energization process. Due to the non-monotonic nature of the ring distribution, at vertical velocities, the magnification produced by this instability is larger than the typical bi-Maxwellian anisotropy distribution because the wave can maintain resonance over a longer portion of its orbit.</description><identifier>ISSN: 0004-640X</identifier><identifier>EISSN: 1572-946X</identifier><identifier>DOI: 10.1007/s10509-018-3466-z</identifier><language>eng</language><publisher>Dordrecht: Springer Netherlands</publisher><subject>Activation ; Anisotropy ; Astrobiology ; Astronomy ; Astrophysics ; Astrophysics and Astroparticles ; Celestial bodies ; Cosmology ; Doppler effect ; Electric fields ; Electron acceleration ; Electron density ; Electron effects ; Emission analysis ; Flux density ; Instability ; Magnetic fields ; Magnetic resonance ; Magnetism ; Magnetosphere ; Mercury ; Observations and Techniques ; Orbital resonances (celestial mechanics) ; Original Article ; Physics ; Physics and Astronomy ; Planetary magnetospheres ; Planets ; Relativistic plasmas ; Saturn ; Solar wind ; Solar wind velocity ; Space Exploration and Astronautics ; Space Sciences (including Extraterrestrial Physics ; Spacecraft ; Temperature effects ; Upstream ; Vertical distribution ; Vertical velocities ; Wave dispersion ; Wave interaction ; Wave propagation ; Whistler waves ; Whistlers ; Wind speed</subject><ispartof>Astrophysics and space science, 2018-12, Vol.363 (12), p.1, Article 249</ispartof><rights>Springer Nature B.V. 2018</rights><rights>Astrophysics and Space Science is a copyright of Springer, (2018). All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c316t-ce94527f6c9a5a013e3f91df3d8b8a6780a354362e9139eb84ed838e534729e33</citedby><cites>FETCH-LOGICAL-c316t-ce94527f6c9a5a013e3f91df3d8b8a6780a354362e9139eb84ed838e534729e33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27922,27923</link.rule.ids></links><search><creatorcontrib>Kumari, Jyoti</creatorcontrib><creatorcontrib>Pandey, R. S.</creatorcontrib><title>Whistler mode waves for ring distribution with A.C. electric field in inner magnetosphere of Saturn</title><title>Astrophysics and space science</title><addtitle>Astrophys Space Sci</addtitle><description>Whistler mode waves can propagate upstream without collision impact. They are generated in these areas of vibration. They are known to play a crucial role in thermodynamics and electron acceleration. Sometimes, in some cases, they are seen as waves that strike the wavefront. Mercury, Earth, Venus and Saturn are the planets where whistlers have been recorded in the upstream regions. They are right handed waves and can be left-hand polarized in the frame of spacecraft due to the strong negative Doppler shift. The weaker Doppler shift owes to the large angle between magnetic field vectors at 10 AU (Astronomical unit) and the solar wind velocity. These waves propagate with an angle between 10 to 60 degrees to background magnetic field. In the present paper, we took an advantage of Cassini present in the Saturnian magnetosphere to explore the whistler mode wave’s importance. A dispersion relation for obliquely as well as for whistler waves propagating perpendicular to the magnetic field, has been applied to Saturnian magnetosphere. Using the observations made by Voyager and Cassini, growth rate has been determined for non-relativistic plasma. Whistler waves are excited by temperature anisotropy, where the vertical temperature is higher than the parallel temperature. The effect of electron density, temperature anisotropy, energy density with some other parameters on the growth of whistler mode emission is studied. The result is found to be in good agreement with observations. Whistler mode wave interaction with particles basically emphasizes on the increase (decrease) in the energy of resonant particles and this variation is related to the transfer of energy to (from) other resonant particle group where the wave is the mediator of the energization process. Due to the non-monotonic nature of the ring distribution, at vertical velocities, the magnification produced by this instability is larger than the typical bi-Maxwellian anisotropy distribution because the wave can maintain resonance over a longer portion of its orbit.</description><subject>Activation</subject><subject>Anisotropy</subject><subject>Astrobiology</subject><subject>Astronomy</subject><subject>Astrophysics</subject><subject>Astrophysics and Astroparticles</subject><subject>Celestial bodies</subject><subject>Cosmology</subject><subject>Doppler effect</subject><subject>Electric fields</subject><subject>Electron acceleration</subject><subject>Electron density</subject><subject>Electron effects</subject><subject>Emission analysis</subject><subject>Flux density</subject><subject>Instability</subject><subject>Magnetic fields</subject><subject>Magnetic resonance</subject><subject>Magnetism</subject><subject>Magnetosphere</subject><subject>Mercury</subject><subject>Observations and Techniques</subject><subject>Orbital resonances (celestial mechanics)</subject><subject>Original Article</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Planetary magnetospheres</subject><subject>Planets</subject><subject>Relativistic plasmas</subject><subject>Saturn</subject><subject>Solar wind</subject><subject>Solar wind velocity</subject><subject>Space Exploration and Astronautics</subject><subject>Space Sciences (including Extraterrestrial Physics</subject><subject>Spacecraft</subject><subject>Temperature effects</subject><subject>Upstream</subject><subject>Vertical distribution</subject><subject>Vertical velocities</subject><subject>Wave dispersion</subject><subject>Wave interaction</subject><subject>Wave propagation</subject><subject>Whistler waves</subject><subject>Whistlers</subject><subject>Wind speed</subject><issn>0004-640X</issn><issn>1572-946X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp1kEtLAzEUhYMoWKs_wF3A9dRk8pjJshRfUHChYnchnblpU6aTMZkq9tebYQRXwoXLfZxz4EPompIZJaS4jZQIojJCy4xxKbPjCZpQUeSZ4nJ1iiaEEJ5JTlbn6CLGXRqVVMUEVe9bF_sGAt77GvCX-YSIrQ84uHaD63QLbn3onW_xl-u3eD5bzDA0UKV9ha2DpsauTdUOFmbTQu9jt4UA2Fv8YvpDaC_RmTVNhKvfPkVv93evi8ds-fzwtJgvs4pR2WcVKC7ywspKGWEIZcCsorVldbkujSxKYpjgTOagKFOwLjnUJStBMF7kChibopvRtwv-4wCx1zuf4lOkzinLRSFFIdIXHb-q4GMMYHUX3N6Eb02JHljqkaVOLPXAUh-TJh81sRu4QPhz_l_0A1Znd7c</recordid><startdate>20181201</startdate><enddate>20181201</enddate><creator>Kumari, Jyoti</creator><creator>Pandey, R. S.</creator><general>Springer Netherlands</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7TG</scope><scope>7XB</scope><scope>88I</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>ABUWG</scope><scope>AEUYN</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>GNUQQ</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L7M</scope><scope>M2P</scope><scope>P5Z</scope><scope>P62</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>Q9U</scope></search><sort><creationdate>20181201</creationdate><title>Whistler mode waves for ring distribution with A.C. electric field in inner magnetosphere of Saturn</title><author>Kumari, Jyoti ; Pandey, R. S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c316t-ce94527f6c9a5a013e3f91df3d8b8a6780a354362e9139eb84ed838e534729e33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Activation</topic><topic>Anisotropy</topic><topic>Astrobiology</topic><topic>Astronomy</topic><topic>Astrophysics</topic><topic>Astrophysics and Astroparticles</topic><topic>Celestial bodies</topic><topic>Cosmology</topic><topic>Doppler effect</topic><topic>Electric fields</topic><topic>Electron acceleration</topic><topic>Electron density</topic><topic>Electron effects</topic><topic>Emission analysis</topic><topic>Flux density</topic><topic>Instability</topic><topic>Magnetic fields</topic><topic>Magnetic resonance</topic><topic>Magnetism</topic><topic>Magnetosphere</topic><topic>Mercury</topic><topic>Observations and Techniques</topic><topic>Orbital resonances (celestial mechanics)</topic><topic>Original Article</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Planetary magnetospheres</topic><topic>Planets</topic><topic>Relativistic plasmas</topic><topic>Saturn</topic><topic>Solar wind</topic><topic>Solar wind velocity</topic><topic>Space Exploration and Astronautics</topic><topic>Space Sciences (including Extraterrestrial Physics</topic><topic>Spacecraft</topic><topic>Temperature effects</topic><topic>Upstream</topic><topic>Vertical distribution</topic><topic>Vertical velocities</topic><topic>Wave dispersion</topic><topic>Wave interaction</topic><topic>Wave propagation</topic><topic>Whistler waves</topic><topic>Whistlers</topic><topic>Wind speed</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kumari, Jyoti</creatorcontrib><creatorcontrib>Pandey, R. 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S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Whistler mode waves for ring distribution with A.C. electric field in inner magnetosphere of Saturn</atitle><jtitle>Astrophysics and space science</jtitle><stitle>Astrophys Space Sci</stitle><date>2018-12-01</date><risdate>2018</risdate><volume>363</volume><issue>12</issue><spage>1</spage><pages>1-</pages><artnum>249</artnum><issn>0004-640X</issn><eissn>1572-946X</eissn><abstract>Whistler mode waves can propagate upstream without collision impact. They are generated in these areas of vibration. They are known to play a crucial role in thermodynamics and electron acceleration. Sometimes, in some cases, they are seen as waves that strike the wavefront. Mercury, Earth, Venus and Saturn are the planets where whistlers have been recorded in the upstream regions. They are right handed waves and can be left-hand polarized in the frame of spacecraft due to the strong negative Doppler shift. The weaker Doppler shift owes to the large angle between magnetic field vectors at 10 AU (Astronomical unit) and the solar wind velocity. These waves propagate with an angle between 10 to 60 degrees to background magnetic field. In the present paper, we took an advantage of Cassini present in the Saturnian magnetosphere to explore the whistler mode wave’s importance. A dispersion relation for obliquely as well as for whistler waves propagating perpendicular to the magnetic field, has been applied to Saturnian magnetosphere. Using the observations made by Voyager and Cassini, growth rate has been determined for non-relativistic plasma. Whistler waves are excited by temperature anisotropy, where the vertical temperature is higher than the parallel temperature. The effect of electron density, temperature anisotropy, energy density with some other parameters on the growth of whistler mode emission is studied. The result is found to be in good agreement with observations. Whistler mode wave interaction with particles basically emphasizes on the increase (decrease) in the energy of resonant particles and this variation is related to the transfer of energy to (from) other resonant particle group where the wave is the mediator of the energization process. Due to the non-monotonic nature of the ring distribution, at vertical velocities, the magnification produced by this instability is larger than the typical bi-Maxwellian anisotropy distribution because the wave can maintain resonance over a longer portion of its orbit.</abstract><cop>Dordrecht</cop><pub>Springer Netherlands</pub><doi>10.1007/s10509-018-3466-z</doi></addata></record> |
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subjects | Activation Anisotropy Astrobiology Astronomy Astrophysics Astrophysics and Astroparticles Celestial bodies Cosmology Doppler effect Electric fields Electron acceleration Electron density Electron effects Emission analysis Flux density Instability Magnetic fields Magnetic resonance Magnetism Magnetosphere Mercury Observations and Techniques Orbital resonances (celestial mechanics) Original Article Physics Physics and Astronomy Planetary magnetospheres Planets Relativistic plasmas Saturn Solar wind Solar wind velocity Space Exploration and Astronautics Space Sciences (including Extraterrestrial Physics Spacecraft Temperature effects Upstream Vertical distribution Vertical velocities Wave dispersion Wave interaction Wave propagation Whistler waves Whistlers Wind speed |
title | Whistler mode waves for ring distribution with A.C. electric field in inner magnetosphere of Saturn |
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