Rayleigh‐Taylor Instability Observed at the Dayside Magnetopause Under Northward Interplanetary Magnetic Field

Under northward interplanetary magnetic field, periodical fluctuations with the period of 85 s have been observed by one of the Time History of Events and Macroscale Interactions during Substorms spacecraft at the dayside magnetopause when the solar wind dynamic pressure suddenly dropped. The observ...

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Veröffentlicht in:Journal of geophysical research. Space physics 2023-07, Vol.128 (7), p.n/a
Hauptverfasser: Yan, G. Q., Parks, G. K., Mozer, F. S., Goldstein, M. L., Chen, T., Liu, Y.
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container_issue 7
container_start_page
container_title Journal of geophysical research. Space physics
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creator Yan, G. Q.
Parks, G. K.
Mozer, F. S.
Goldstein, M. L.
Chen, T.
Liu, Y.
description Under northward interplanetary magnetic field, periodical fluctuations with the period of 85 s have been observed by one of the Time History of Events and Macroscale Interactions during Substorms spacecraft at the dayside magnetopause when the solar wind dynamic pressure suddenly dropped. The observed magnetic field distortions, characterized by the compression of the main component as well as the flapping of the perpendicular components, are in line with the theoretical predictions of the Rayleigh‐Taylor (R‐T) instability excited at the magnetopause. With the convective electric field and the mean electric field removed, the perturbations in the electric field are identified as typical two sinusoidal signals with a 90° phase difference, consistent with previous prediction of the attendant electrostatic field arising from the R‐T instability. The transverse motions of the plasmas resulting from the electric drifting driven by the electrostatic field are observed both in pitch‐angle distributions and in distribution functions. The growth rate of the R‐T instability is about 43 s, implying that the instability has time to grow during the disturbances. Using the Gauss theorem, the calculated net charge density based on the electric field observation is one part of 27 compared to the totally observed plasma density, indicating that only a tiny fraction of the charge separates to set up the electrostatic field, which is due to a collective effect in the plasma. Plain Language Summary The magnetopause, the outmost edge that our planet's intrinsic magnetic field reaches, is always in motion. The macroscopic acceleration at the magnetopause is sometimes as large as a few km/s2. Theoretically, such an acceleration of the boundary can facilitate an instability in the motion of the interface, the R‐T instability. Such an instability can, in turn, cause a transfer of plasma across the magnetopause, from solar wind into the near‐Earth space. If the resulting particles are sufficiently energetic, operations of many satellites in space can be threatened. However, details of how the instability operates at the magnetopause have been neither verified nor observed in spacecraft observations. Recent measurements from NASA's Time History of Events and Macroscale Interactions during Substorms mission indicate that the R‐T instability can be excited at the magnetopause, and many details of the instability, including those of its electric field and plasma transport across the ma
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Q. ; Parks, G. K. ; Mozer, F. S. ; Goldstein, M. L. ; Chen, T. ; Liu, Y.</creator><creatorcontrib>Yan, G. Q. ; Parks, G. K. ; Mozer, F. S. ; Goldstein, M. L. ; Chen, T. ; Liu, Y.</creatorcontrib><description>Under northward interplanetary magnetic field, periodical fluctuations with the period of 85 s have been observed by one of the Time History of Events and Macroscale Interactions during Substorms spacecraft at the dayside magnetopause when the solar wind dynamic pressure suddenly dropped. The observed magnetic field distortions, characterized by the compression of the main component as well as the flapping of the perpendicular components, are in line with the theoretical predictions of the Rayleigh‐Taylor (R‐T) instability excited at the magnetopause. With the convective electric field and the mean electric field removed, the perturbations in the electric field are identified as typical two sinusoidal signals with a 90° phase difference, consistent with previous prediction of the attendant electrostatic field arising from the R‐T instability. The transverse motions of the plasmas resulting from the electric drifting driven by the electrostatic field are observed both in pitch‐angle distributions and in distribution functions. The growth rate of the R‐T instability is about 43 s, implying that the instability has time to grow during the disturbances. Using the Gauss theorem, the calculated net charge density based on the electric field observation is one part of 27 compared to the totally observed plasma density, indicating that only a tiny fraction of the charge separates to set up the electrostatic field, which is due to a collective effect in the plasma. Plain Language Summary The magnetopause, the outmost edge that our planet's intrinsic magnetic field reaches, is always in motion. The macroscopic acceleration at the magnetopause is sometimes as large as a few km/s2. Theoretically, such an acceleration of the boundary can facilitate an instability in the motion of the interface, the R‐T instability. Such an instability can, in turn, cause a transfer of plasma across the magnetopause, from solar wind into the near‐Earth space. If the resulting particles are sufficiently energetic, operations of many satellites in space can be threatened. However, details of how the instability operates at the magnetopause have been neither verified nor observed in spacecraft observations. Recent measurements from NASA's Time History of Events and Macroscale Interactions during Substorms mission indicate that the R‐T instability can be excited at the magnetopause, and many details of the instability, including those of its electric field and plasma transport across the magnetopause appear to be verified in those observations. Key Points 85‐s periodic fluctuations with plasma transport are observed at the magnetopause when solar wind dynamic pressure decreases abruptly Magnetic field is found fluted along the mean field direction and meandering along the perpendicular direction The attendant electric field of the Rayleigh‐Taylor instability, as well as the resultant cross‐field drift of the plasma, are also identified</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1029/2023JA031461</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Charge density ; Distribution functions ; Dynamic pressure ; Electric fields ; electrostatic field ; Flapping ; Instability ; Interface stability ; Interplanetary magnetic field ; Magnetic fields ; Magnetopause ; Motion stability ; Perturbation ; Plasma ; Plasma density ; plasma transport ; Rayleigh‐Taylor instability ; Solar wind ; Spacecraft ; Taylor instability</subject><ispartof>Journal of geophysical research. 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K.</creatorcontrib><creatorcontrib>Mozer, F. S.</creatorcontrib><creatorcontrib>Goldstein, M. L.</creatorcontrib><creatorcontrib>Chen, T.</creatorcontrib><creatorcontrib>Liu, Y.</creatorcontrib><title>Rayleigh‐Taylor Instability Observed at the Dayside Magnetopause Under Northward Interplanetary Magnetic Field</title><title>Journal of geophysical research. Space physics</title><description>Under northward interplanetary magnetic field, periodical fluctuations with the period of 85 s have been observed by one of the Time History of Events and Macroscale Interactions during Substorms spacecraft at the dayside magnetopause when the solar wind dynamic pressure suddenly dropped. The observed magnetic field distortions, characterized by the compression of the main component as well as the flapping of the perpendicular components, are in line with the theoretical predictions of the Rayleigh‐Taylor (R‐T) instability excited at the magnetopause. With the convective electric field and the mean electric field removed, the perturbations in the electric field are identified as typical two sinusoidal signals with a 90° phase difference, consistent with previous prediction of the attendant electrostatic field arising from the R‐T instability. The transverse motions of the plasmas resulting from the electric drifting driven by the electrostatic field are observed both in pitch‐angle distributions and in distribution functions. The growth rate of the R‐T instability is about 43 s, implying that the instability has time to grow during the disturbances. Using the Gauss theorem, the calculated net charge density based on the electric field observation is one part of 27 compared to the totally observed plasma density, indicating that only a tiny fraction of the charge separates to set up the electrostatic field, which is due to a collective effect in the plasma. Plain Language Summary The magnetopause, the outmost edge that our planet's intrinsic magnetic field reaches, is always in motion. The macroscopic acceleration at the magnetopause is sometimes as large as a few km/s2. Theoretically, such an acceleration of the boundary can facilitate an instability in the motion of the interface, the R‐T instability. Such an instability can, in turn, cause a transfer of plasma across the magnetopause, from solar wind into the near‐Earth space. If the resulting particles are sufficiently energetic, operations of many satellites in space can be threatened. However, details of how the instability operates at the magnetopause have been neither verified nor observed in spacecraft observations. Recent measurements from NASA's Time History of Events and Macroscale Interactions during Substorms mission indicate that the R‐T instability can be excited at the magnetopause, and many details of the instability, including those of its electric field and plasma transport across the magnetopause appear to be verified in those observations. Key Points 85‐s periodic fluctuations with plasma transport are observed at the magnetopause when solar wind dynamic pressure decreases abruptly Magnetic field is found fluted along the mean field direction and meandering along the perpendicular direction The attendant electric field of the Rayleigh‐Taylor instability, as well as the resultant cross‐field drift of the plasma, are also identified</description><subject>Charge density</subject><subject>Distribution functions</subject><subject>Dynamic pressure</subject><subject>Electric fields</subject><subject>electrostatic field</subject><subject>Flapping</subject><subject>Instability</subject><subject>Interface stability</subject><subject>Interplanetary magnetic field</subject><subject>Magnetic fields</subject><subject>Magnetopause</subject><subject>Motion stability</subject><subject>Perturbation</subject><subject>Plasma</subject><subject>Plasma density</subject><subject>plasma transport</subject><subject>Rayleigh‐Taylor instability</subject><subject>Solar wind</subject><subject>Spacecraft</subject><subject>Taylor instability</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kM1OwkAUhSdGEwmy8wEmcSs6vy2zJCgIQUkIrJtp5xaG1LbOFEl3PoLP6JM4BE1ceTf35ObLuScHoWtK7ihh6p4RxmdDwqmI6BnqMBqpvhKEnf9qPiCXqOf9joQZhBOVHVQvdVuA3Wy_Pj5XQVYOT0vf6NQWtmnxIvXg3sFg3eBmC_hBt94awM96U0JT1XrvAa9LAw6_VK7ZHrQzwaABVxc6ENq1P6zN8NhCYa7QRa4LD72f3UXr8eNq9NSfLybT0XDezziJSV9HgnMmpIkyksfUmCyNgLE4FSmhXDIlteFcE0FkrE0stASWE5ZxqQRkkeJddHPyrV31tgffJLtq78rwMmEDQRWjIj5Stycqc5X3DvKkdvY1pE4oSY61Jn9rDTg_4QdbQPsvm8wmy6GMFSP8G9JGefo</recordid><startdate>202307</startdate><enddate>202307</enddate><creator>Yan, G. 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Q.</creatorcontrib><creatorcontrib>Parks, G. K.</creatorcontrib><creatorcontrib>Mozer, F. S.</creatorcontrib><creatorcontrib>Goldstein, M. L.</creatorcontrib><creatorcontrib>Chen, T.</creatorcontrib><creatorcontrib>Liu, Y.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological &amp; Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological &amp; Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yan, G. Q.</au><au>Parks, G. K.</au><au>Mozer, F. S.</au><au>Goldstein, M. L.</au><au>Chen, T.</au><au>Liu, Y.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Rayleigh‐Taylor Instability Observed at the Dayside Magnetopause Under Northward Interplanetary Magnetic Field</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2023-07</date><risdate>2023</risdate><volume>128</volume><issue>7</issue><epage>n/a</epage><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>Under northward interplanetary magnetic field, periodical fluctuations with the period of 85 s have been observed by one of the Time History of Events and Macroscale Interactions during Substorms spacecraft at the dayside magnetopause when the solar wind dynamic pressure suddenly dropped. The observed magnetic field distortions, characterized by the compression of the main component as well as the flapping of the perpendicular components, are in line with the theoretical predictions of the Rayleigh‐Taylor (R‐T) instability excited at the magnetopause. With the convective electric field and the mean electric field removed, the perturbations in the electric field are identified as typical two sinusoidal signals with a 90° phase difference, consistent with previous prediction of the attendant electrostatic field arising from the R‐T instability. The transverse motions of the plasmas resulting from the electric drifting driven by the electrostatic field are observed both in pitch‐angle distributions and in distribution functions. The growth rate of the R‐T instability is about 43 s, implying that the instability has time to grow during the disturbances. Using the Gauss theorem, the calculated net charge density based on the electric field observation is one part of 27 compared to the totally observed plasma density, indicating that only a tiny fraction of the charge separates to set up the electrostatic field, which is due to a collective effect in the plasma. Plain Language Summary The magnetopause, the outmost edge that our planet's intrinsic magnetic field reaches, is always in motion. The macroscopic acceleration at the magnetopause is sometimes as large as a few km/s2. Theoretically, such an acceleration of the boundary can facilitate an instability in the motion of the interface, the R‐T instability. Such an instability can, in turn, cause a transfer of plasma across the magnetopause, from solar wind into the near‐Earth space. If the resulting particles are sufficiently energetic, operations of many satellites in space can be threatened. However, details of how the instability operates at the magnetopause have been neither verified nor observed in spacecraft observations. Recent measurements from NASA's Time History of Events and Macroscale Interactions during Substorms mission indicate that the R‐T instability can be excited at the magnetopause, and many details of the instability, including those of its electric field and plasma transport across the magnetopause appear to be verified in those observations. Key Points 85‐s periodic fluctuations with plasma transport are observed at the magnetopause when solar wind dynamic pressure decreases abruptly Magnetic field is found fluted along the mean field direction and meandering along the perpendicular direction The attendant electric field of the Rayleigh‐Taylor instability, as well as the resultant cross‐field drift of the plasma, are also identified</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2023JA031461</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0002-5317-988X</orcidid><orcidid>https://orcid.org/0000-0001-5580-5621</orcidid><orcidid>https://orcid.org/0000-0001-9790-2358</orcidid><orcidid>https://orcid.org/0000-0002-8608-0528</orcidid><orcidid>https://orcid.org/0000-0002-2011-8140</orcidid></addata></record>
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subjects Charge density
Distribution functions
Dynamic pressure
Electric fields
electrostatic field
Flapping
Instability
Interface stability
Interplanetary magnetic field
Magnetic fields
Magnetopause
Motion stability
Perturbation
Plasma
Plasma density
plasma transport
Rayleigh‐Taylor instability
Solar wind
Spacecraft
Taylor instability
title Rayleigh‐Taylor Instability Observed at the Dayside Magnetopause Under Northward Interplanetary Magnetic Field
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