Motion of Classic and Spontaneous Hot Flow Anomalies Observed by Cluster

The propagation characteristics of hot flow anomalies (HFAs) near the Earth's bow shock are investigated, using observations from the Cluster spacecraft. A data set comprised of 19 classic HFAs (associated with tangential discontinuities, TDs) and 23 spontaneous HFAs (SHFAs, formed in the absen...

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Veröffentlicht in:Journal of geophysical research. Space physics 2021-11, Vol.126 (11), p.n/a
Hauptverfasser: Zhu, Xiaoqiong, Wang, Mengmeng, Shi, Quanqi, Zhang, Hui, Tian, Anmin, Yao, Shutao, Guo, Ruilong, Liu, Ji, Bai, Shichen, Degeling, Alexander William, Zhang, Shuai, Niu, Zhe, Zhao, Jinyan, Xiao, Yuchen, Shang, Wensai
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container_issue 11
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container_title Journal of geophysical research. Space physics
container_volume 126
creator Zhu, Xiaoqiong
Wang, Mengmeng
Shi, Quanqi
Zhang, Hui
Tian, Anmin
Yao, Shutao
Guo, Ruilong
Liu, Ji
Bai, Shichen
Degeling, Alexander William
Zhang, Shuai
Niu, Zhe
Zhao, Jinyan
Xiao, Yuchen
Shang, Wensai
description The propagation characteristics of hot flow anomalies (HFAs) near the Earth's bow shock are investigated, using observations from the Cluster spacecraft. A data set comprised of 19 classic HFAs (associated with tangential discontinuities, TDs) and 23 spontaneous HFAs (SHFAs, formed in the absence of solar wind discontinuities) was analyzed. For each event, the propagation velocity and normal of leading and trailing HFA edges were calculated using multiple multi‐point satellite analysis methods. For classic HFAs, 93% of the events have leading edge (LE) normal directions within 30° of the normal direction of the driving TDs. For SHFAs, in 74% of the events, the angle between the normal of an SHFA's edges and background magnetic field is in the range of 70°–110° and no angle is in the ranges of 0°–20° and 160°–180°. These results indicate that the LEs of the classic HFAs propagate along the same direction as the driving TDs and most SHFAs propagate quasi‐perpendicular to the background magnetic field and no SHFAs propagate parallel or anti‐parallel to the background magnetic field. Moreover, according to the velocity of HFAs' edges, we find that all classic HFAs and SHFAs' edges propagate toward the Earth in the spacecraft frame as expected and 5 out of 7 SHFAs are contracting and no expanding SHFAs are found. This study provides key parameters to help understand how HFAs disturb the magnetosphere. Plain Language Summary Hot flow anomalies (HFAs) are transient phenomena widely observed in the solar wind upstream of the Earth's bow shock. They can disturb the local bow shock and magnetopause, generate field line resonances in the magnetosphere and associated auroral brightening in the ionosphere. The propagation of HFAs can affect the features of the above disturbances. However, there are no statistical studies about the propagation of HFAs using multiple multi‐satellite analysis methods. This study investigates the propagation of two types of HFAs, so‐called “classic” HFAs and “spontaneous” HFAs (SHFAs), by calculating the velocity of their edges using multiple multipoint satellite analysis methods. We find that the leading edges of classic HFAs move along the normal direction of the driving discontinuities (consistent with previous simulations). Most SHFAs propagate quasi‐perpendicular to the background magnetic field. We discuss the propagation of the classic HFAs and SHFAs and the factors that may affect their propagation. This will help understand the ev
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A data set comprised of 19 classic HFAs (associated with tangential discontinuities, TDs) and 23 spontaneous HFAs (SHFAs, formed in the absence of solar wind discontinuities) was analyzed. For each event, the propagation velocity and normal of leading and trailing HFA edges were calculated using multiple multi‐point satellite analysis methods. For classic HFAs, 93% of the events have leading edge (LE) normal directions within 30° of the normal direction of the driving TDs. For SHFAs, in 74% of the events, the angle between the normal of an SHFA's edges and background magnetic field is in the range of 70°–110° and no angle is in the ranges of 0°–20° and 160°–180°. These results indicate that the LEs of the classic HFAs propagate along the same direction as the driving TDs and most SHFAs propagate quasi‐perpendicular to the background magnetic field and no SHFAs propagate parallel or anti‐parallel to the background magnetic field. Moreover, according to the velocity of HFAs' edges, we find that all classic HFAs and SHFAs' edges propagate toward the Earth in the spacecraft frame as expected and 5 out of 7 SHFAs are contracting and no expanding SHFAs are found. This study provides key parameters to help understand how HFAs disturb the magnetosphere. Plain Language Summary Hot flow anomalies (HFAs) are transient phenomena widely observed in the solar wind upstream of the Earth's bow shock. They can disturb the local bow shock and magnetopause, generate field line resonances in the magnetosphere and associated auroral brightening in the ionosphere. The propagation of HFAs can affect the features of the above disturbances. However, there are no statistical studies about the propagation of HFAs using multiple multi‐satellite analysis methods. This study investigates the propagation of two types of HFAs, so‐called “classic” HFAs and “spontaneous” HFAs (SHFAs), by calculating the velocity of their edges using multiple multipoint satellite analysis methods. We find that the leading edges of classic HFAs move along the normal direction of the driving discontinuities (consistent with previous simulations). Most SHFAs propagate quasi‐perpendicular to the background magnetic field. We discuss the propagation of the classic HFAs and SHFAs and the factors that may affect their propagation. This will help understand the evolution and energy transfer of the structures and aid predictions of the propagation of HFA‐induced disturbances in the magnetosheath, magnetosphere, and ionosphere. Key Points The leading edges of classic hot flow anomalies (HFAs) move along the normal direction of the driving tangential discontinuities Seventy‐four percent of the spontaneous HFAs propagate quasi‐perpendicular to the background magnetic field Most spontaneous HFAs are contracting, and no expanding spontaneous HFAs are found</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1029/2021JA029418</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Anomalies ; Brightening ; Cluster spacecraft ; Clusters ; Discontinuity ; Disturbances ; Earth ; Energy transfer ; hot flow anomalies ; Ionosphere ; Ionospheric propagation ; Leading edges ; Magnetic fields ; Magnetopause ; Magnetosheath ; Magnetospheres ; Mathematical analysis ; Propagation ; propagation properties ; Propagation velocity ; Satellites ; Solar wind ; Spacecraft ; spontaneous hot flow anomalies</subject><ispartof>Journal of geophysical research. 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Space physics</title><description>The propagation characteristics of hot flow anomalies (HFAs) near the Earth's bow shock are investigated, using observations from the Cluster spacecraft. A data set comprised of 19 classic HFAs (associated with tangential discontinuities, TDs) and 23 spontaneous HFAs (SHFAs, formed in the absence of solar wind discontinuities) was analyzed. For each event, the propagation velocity and normal of leading and trailing HFA edges were calculated using multiple multi‐point satellite analysis methods. For classic HFAs, 93% of the events have leading edge (LE) normal directions within 30° of the normal direction of the driving TDs. For SHFAs, in 74% of the events, the angle between the normal of an SHFA's edges and background magnetic field is in the range of 70°–110° and no angle is in the ranges of 0°–20° and 160°–180°. These results indicate that the LEs of the classic HFAs propagate along the same direction as the driving TDs and most SHFAs propagate quasi‐perpendicular to the background magnetic field and no SHFAs propagate parallel or anti‐parallel to the background magnetic field. Moreover, according to the velocity of HFAs' edges, we find that all classic HFAs and SHFAs' edges propagate toward the Earth in the spacecraft frame as expected and 5 out of 7 SHFAs are contracting and no expanding SHFAs are found. This study provides key parameters to help understand how HFAs disturb the magnetosphere. Plain Language Summary Hot flow anomalies (HFAs) are transient phenomena widely observed in the solar wind upstream of the Earth's bow shock. They can disturb the local bow shock and magnetopause, generate field line resonances in the magnetosphere and associated auroral brightening in the ionosphere. The propagation of HFAs can affect the features of the above disturbances. 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Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhu, Xiaoqiong</au><au>Wang, Mengmeng</au><au>Shi, Quanqi</au><au>Zhang, Hui</au><au>Tian, Anmin</au><au>Yao, Shutao</au><au>Guo, Ruilong</au><au>Liu, Ji</au><au>Bai, Shichen</au><au>Degeling, Alexander William</au><au>Zhang, Shuai</au><au>Niu, Zhe</au><au>Zhao, Jinyan</au><au>Xiao, Yuchen</au><au>Shang, Wensai</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Motion of Classic and Spontaneous Hot Flow Anomalies Observed by Cluster</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2021-11</date><risdate>2021</risdate><volume>126</volume><issue>11</issue><epage>n/a</epage><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>The propagation characteristics of hot flow anomalies (HFAs) near the Earth's bow shock are investigated, using observations from the Cluster spacecraft. A data set comprised of 19 classic HFAs (associated with tangential discontinuities, TDs) and 23 spontaneous HFAs (SHFAs, formed in the absence of solar wind discontinuities) was analyzed. For each event, the propagation velocity and normal of leading and trailing HFA edges were calculated using multiple multi‐point satellite analysis methods. For classic HFAs, 93% of the events have leading edge (LE) normal directions within 30° of the normal direction of the driving TDs. For SHFAs, in 74% of the events, the angle between the normal of an SHFA's edges and background magnetic field is in the range of 70°–110° and no angle is in the ranges of 0°–20° and 160°–180°. These results indicate that the LEs of the classic HFAs propagate along the same direction as the driving TDs and most SHFAs propagate quasi‐perpendicular to the background magnetic field and no SHFAs propagate parallel or anti‐parallel to the background magnetic field. Moreover, according to the velocity of HFAs' edges, we find that all classic HFAs and SHFAs' edges propagate toward the Earth in the spacecraft frame as expected and 5 out of 7 SHFAs are contracting and no expanding SHFAs are found. This study provides key parameters to help understand how HFAs disturb the magnetosphere. Plain Language Summary Hot flow anomalies (HFAs) are transient phenomena widely observed in the solar wind upstream of the Earth's bow shock. They can disturb the local bow shock and magnetopause, generate field line resonances in the magnetosphere and associated auroral brightening in the ionosphere. The propagation of HFAs can affect the features of the above disturbances. However, there are no statistical studies about the propagation of HFAs using multiple multi‐satellite analysis methods. This study investigates the propagation of two types of HFAs, so‐called “classic” HFAs and “spontaneous” HFAs (SHFAs), by calculating the velocity of their edges using multiple multipoint satellite analysis methods. We find that the leading edges of classic HFAs move along the normal direction of the driving discontinuities (consistent with previous simulations). Most SHFAs propagate quasi‐perpendicular to the background magnetic field. We discuss the propagation of the classic HFAs and SHFAs and the factors that may affect their propagation. This will help understand the evolution and energy transfer of the structures and aid predictions of the propagation of HFA‐induced disturbances in the magnetosheath, magnetosphere, and ionosphere. Key Points The leading edges of classic hot flow anomalies (HFAs) move along the normal direction of the driving tangential discontinuities Seventy‐four percent of the spontaneous HFAs propagate quasi‐perpendicular to the background magnetic field Most spontaneous HFAs are contracting, and no expanding spontaneous HFAs are found</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2021JA029418</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0002-6059-2963</orcidid><orcidid>https://orcid.org/0000-0001-7338-9270</orcidid><orcidid>https://orcid.org/0000-0001-8937-7987</orcidid><orcidid>https://orcid.org/0000-0001-5346-7112</orcidid><orcidid>https://orcid.org/0000-0002-4351-551X</orcidid><orcidid>https://orcid.org/0000-0002-7078-8249</orcidid><orcidid>https://orcid.org/0000-0002-7125-0942</orcidid><orcidid>https://orcid.org/0000-0001-6835-4751</orcidid><orcidid>https://orcid.org/0000-0002-7686-1910</orcidid><orcidid>https://orcid.org/0000-0001-6230-4040</orcidid><orcidid>https://orcid.org/0000-0001-6648-8908</orcidid></addata></record>
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subjects Anomalies
Brightening
Cluster spacecraft
Clusters
Discontinuity
Disturbances
Earth
Energy transfer
hot flow anomalies
Ionosphere
Ionospheric propagation
Leading edges
Magnetic fields
Magnetopause
Magnetosheath
Magnetospheres
Mathematical analysis
Propagation
propagation properties
Propagation velocity
Satellites
Solar wind
Spacecraft
spontaneous hot flow anomalies
title Motion of Classic and Spontaneous Hot Flow Anomalies Observed by Cluster
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