MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991
Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combine...
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Veröffentlicht in: | Journal of geophysical research. Space physics 2016-05, Vol.121 (5), p.4397-4408 |
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creator | Bandić, Mario Verbanac, Giuli Moldwin, Mark B. Pierrard, Viviane Piredda, Giovanni |
description | Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combines different physical mechanisms which run magnetospheric activity), and (b) geomagnetic indices Dst, Ap, and AE. The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. The decrease in the convection electric field places the bulge toward midnight. These results are compared and discussed in regard to past works. Our study shows that the time delays in the plasmapause response are a function of MLT and suggests that the plasmapause is formed by the mechanism of interchange instability motion. We observed that any change quickly propagates across dawn to noon, and then at lower rate toward midnight. The results further indicate that the instability may propagate much faster during solar maximum than around solar minimum. This study contributes to the determination of the MLT dependence of the plasmapause and to constrain physical mechanism by which the plasmapause is formed.
Key Points
The delay times of Lpp to the arrival of Lpp indicators is a function of MLT
The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability
At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight |
doi_str_mv | 10.1002/2015JA022278 |
format | Article |
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Key Points
The delay times of Lpp to the arrival of Lpp indicators is a function of MLT
The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability
At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1002/2015JA022278</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Charged particles ; Convection ; Correlation analysis ; CRESS satellite ; CRRES (satellite) ; Delay ; Dependence ; Electric fields ; Geomagnetic activity ; Geomagnetism ; Instability ; Interplanetary magnetic field ; Interplanetary magnetic fields ; Magnetic fields ; Magnetism ; Magnetospheres ; Mathematical models ; Motion stability ; Parameters ; Plasmapause ; Solar cycle ; Solar maximum ; Solar minimum ; Solar wind ; Solar wind parameters ; Solar wind velocity ; Stability ; Wind speed</subject><ispartof>Journal of geophysical research. Space physics, 2016-05, Vol.121 (5), p.4397-4408</ispartof><rights>2016. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c5052-dafc7aeba5ec5cb8e6da986b2d42d7675dcde4af62b3ad7ca98e0fe2c45185c83</citedby><cites>FETCH-LOGICAL-c5052-dafc7aeba5ec5cb8e6da986b2d42d7675dcde4af62b3ad7ca98e0fe2c45185c83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2F2015JA022278$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2F2015JA022278$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>315,782,786,1419,1435,27931,27932,45581,45582,46416,46840</link.rule.ids></links><search><creatorcontrib>Bandić, Mario</creatorcontrib><creatorcontrib>Verbanac, Giuli</creatorcontrib><creatorcontrib>Moldwin, Mark B.</creatorcontrib><creatorcontrib>Pierrard, Viviane</creatorcontrib><creatorcontrib>Piredda, Giovanni</creatorcontrib><title>MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991</title><title>Journal of geophysical research. Space physics</title><description>Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combines different physical mechanisms which run magnetospheric activity), and (b) geomagnetic indices Dst, Ap, and AE. The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. The decrease in the convection electric field places the bulge toward midnight. These results are compared and discussed in regard to past works. Our study shows that the time delays in the plasmapause response are a function of MLT and suggests that the plasmapause is formed by the mechanism of interchange instability motion. We observed that any change quickly propagates across dawn to noon, and then at lower rate toward midnight. The results further indicate that the instability may propagate much faster during solar maximum than around solar minimum. This study contributes to the determination of the MLT dependence of the plasmapause and to constrain physical mechanism by which the plasmapause is formed.
Key Points
The delay times of Lpp to the arrival of Lpp indicators is a function of MLT
The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability
At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight</description><subject>Charged particles</subject><subject>Convection</subject><subject>Correlation analysis</subject><subject>CRESS satellite</subject><subject>CRRES (satellite)</subject><subject>Delay</subject><subject>Dependence</subject><subject>Electric fields</subject><subject>Geomagnetic activity</subject><subject>Geomagnetism</subject><subject>Instability</subject><subject>Interplanetary magnetic field</subject><subject>Interplanetary magnetic fields</subject><subject>Magnetic fields</subject><subject>Magnetism</subject><subject>Magnetospheres</subject><subject>Mathematical models</subject><subject>Motion stability</subject><subject>Parameters</subject><subject>Plasmapause</subject><subject>Solar cycle</subject><subject>Solar maximum</subject><subject>Solar minimum</subject><subject>Solar wind</subject><subject>Solar wind parameters</subject><subject>Solar wind velocity</subject><subject>Stability</subject><subject>Wind speed</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqN0c1q3DAQB3BTUmhIc-sDCHrJYbeVxpYs5bYs-WjYENikZzOWxomCV3YsbzZ76zvkDfskVdkUQg6huoyY-TEw_LPsi-DfBOfwHbiQFzMOAKX-kO2DUGZqCg57__655p-ywxjveXo6tYTcz54uFzfMUU_BUbDEfGDjHbGBWhx9F-Kd71lN44YosL7FuMIe15EmLHYtDmzjg5swDI7dUrfC20Cjtwzt6B_9uGU1RnKsC2y-XJ5cHzNhDP_96zkV8Tn72GAb6fClHmQ_T09u5ufTxdXZj_lsMbWSS5g6bGyJVKMkK22tSTk0WtXgCnClKqWzjgpsFNQ5utKmIfGGwBZSaGl1fpAd7fb2Q_ewpjhWKx8ttS0G6taxEhqkFKBz8x-Ua1Vow3miX9_Q-249hHRIBSkNU5RlLt5TojTKFEopSGqyU3boYhyoqfrBr3DYVoJXf6OtXkebeL7jG9_S9l1bXZwtZxKkhvwPPhWjdw</recordid><startdate>201605</startdate><enddate>201605</enddate><creator>Bandić, Mario</creator><creator>Verbanac, Giuli</creator><creator>Moldwin, Mark B.</creator><creator>Pierrard, Viviane</creator><creator>Piredda, Giovanni</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope></search><sort><creationdate>201605</creationdate><title>MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991</title><author>Bandić, Mario ; Verbanac, Giuli ; Moldwin, Mark B. ; Pierrard, Viviane ; Piredda, Giovanni</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c5052-dafc7aeba5ec5cb8e6da986b2d42d7675dcde4af62b3ad7ca98e0fe2c45185c83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Charged particles</topic><topic>Convection</topic><topic>Correlation analysis</topic><topic>CRESS satellite</topic><topic>CRRES (satellite)</topic><topic>Delay</topic><topic>Dependence</topic><topic>Electric fields</topic><topic>Geomagnetic activity</topic><topic>Geomagnetism</topic><topic>Instability</topic><topic>Interplanetary magnetic field</topic><topic>Interplanetary magnetic fields</topic><topic>Magnetic fields</topic><topic>Magnetism</topic><topic>Magnetospheres</topic><topic>Mathematical models</topic><topic>Motion stability</topic><topic>Parameters</topic><topic>Plasmapause</topic><topic>Solar cycle</topic><topic>Solar maximum</topic><topic>Solar minimum</topic><topic>Solar wind</topic><topic>Solar wind parameters</topic><topic>Solar wind velocity</topic><topic>Stability</topic><topic>Wind speed</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bandić, Mario</creatorcontrib><creatorcontrib>Verbanac, Giuli</creatorcontrib><creatorcontrib>Moldwin, Mark B.</creatorcontrib><creatorcontrib>Pierrard, Viviane</creatorcontrib><creatorcontrib>Piredda, Giovanni</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & 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>Bandić, Mario</au><au>Verbanac, Giuli</au><au>Moldwin, Mark B.</au><au>Pierrard, Viviane</au><au>Piredda, Giovanni</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2016-05</date><risdate>2016</risdate><volume>121</volume><issue>5</issue><spage>4397</spage><epage>4408</epage><pages>4397-4408</pages><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>Using the database of CRRES in situ observations of the plasmapause crossings, we develop linear and more complex plasmapause models parametrized by (a) solar wind parameters V (solar wind velocity), BV (where B is the magnitude of the interplanetary magnetic field (IMF)), and dΦmp/dt (which combines different physical mechanisms which run magnetospheric activity), and (b) geomagnetic indices Dst, Ap, and AE. The complex models are built by including a first harmonic in magnetic local time (MLT). Our method based on the cross‐correlation analyses provides not only the plasmapause shape for different levels of geomagnetic activity but additionally yields the information of the delays in the MLT response of the plasmapause. All models based on both solar wind parameters and geomagnetic indices indicate the maximal plasmapause extension in the postdusk side at high geomagnetic activity. The decrease in the convection electric field places the bulge toward midnight. These results are compared and discussed in regard to past works. Our study shows that the time delays in the plasmapause response are a function of MLT and suggests that the plasmapause is formed by the mechanism of interchange instability motion. We observed that any change quickly propagates across dawn to noon, and then at lower rate toward midnight. The results further indicate that the instability may propagate much faster during solar maximum than around solar minimum. This study contributes to the determination of the MLT dependence of the plasmapause and to constrain physical mechanism by which the plasmapause is formed.
Key Points
The delay times of Lpp to the arrival of Lpp indicators is a function of MLT
The MLT dependence of plasmapause formation is in agreement with the mechanism of interchange instability
At high geomagnetic activity the Lpp bulge is formed in the postdusk; at low geomagnetic activity the bulge is located close to midnight</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2015JA022278</doi><tpages>12</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Charged particles Convection Correlation analysis CRESS satellite CRRES (satellite) Delay Dependence Electric fields Geomagnetic activity Geomagnetism Instability Interplanetary magnetic field Interplanetary magnetic fields Magnetic fields Magnetism Magnetospheres Mathematical models Motion stability Parameters Plasmapause Solar cycle Solar maximum Solar minimum Solar wind Solar wind parameters Solar wind velocity Stability Wind speed |
title | MLT dependence in the relationship between plasmapause, solar wind, and geomagnetic activity based on CRRES: 1990–1991 |
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