Decoding solar wind‐magnetosphere coupling

We employ a new NARMAX (Nonlinear Auto‐Regressive Moving Average with eXogenous inputs) code to disentangle the time‐varying relationship between the solar wind and SYM‐H. The NARMAX method has previously been used to formulate a Dst model, using a preselected solar wind coupling function. In this w...

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Veröffentlicht in:Space Weather 2016-10, Vol.14 (10), p.724-741
Hauptverfasser: Beharrell, M. J., Honary, F.
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Honary, F.
description We employ a new NARMAX (Nonlinear Auto‐Regressive Moving Average with eXogenous inputs) code to disentangle the time‐varying relationship between the solar wind and SYM‐H. The NARMAX method has previously been used to formulate a Dst model, using a preselected solar wind coupling function. In this work, which uses the higher‐resolution SYM‐H in place of Dst, we are able to reveal the individual components of different solar wind‐magnetosphere interaction processes as they contribute to the geomagnetic disturbance. This is achieved with a graphics processing unit (GPU)‐based NARMAX code that is around 10 orders of magnitude faster than previous efforts from 2005, before general‐purpose programming on GPUs was possible. The algorithm includes a composite cost function, to minimize overfitting, and iterative reorthogonalization, which reduces computational errors in the most critical calculations by a factor of ∼106. The results show that negative deviations in SYM‐H following a southward interplanetary magnetic field (IMF) are first a measure of the increased magnetic flux in the geomagnetic tail, observed with a delay of 20–30 min from the time the solar wind hits the bow shock. Terms with longer delays are found which represent the dipolarization of the magnetotail, the injections of particles into the ring current, and their subsequent loss by flowout through the dayside magnetopause. Our results indicate that the contribution of magnetopause currents to the storm time indices increase with solar wind electric field, E = v × B. This is in agreement with previous studies that have shown that the magnetopause is closer to the Earth when the IMF is in the tangential direction. Key Points Empirical model of SW‐magnetosphere coupling gives insight into the various mechanisms and provides formulas to quantify their effects New GPU‐based NARMAX code is used: 1 million times more precise and 10 billion times faster than previous efforts Very small changes in SYM‐H that occur on short timescales can be accurately reproduced by the model using just solar wind data
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J. ; Honary, F.</creator><creatorcontrib>Beharrell, M. J. ; Honary, F.</creatorcontrib><description>We employ a new NARMAX (Nonlinear Auto‐Regressive Moving Average with eXogenous inputs) code to disentangle the time‐varying relationship between the solar wind and SYM‐H. The NARMAX method has previously been used to formulate a Dst model, using a preselected solar wind coupling function. In this work, which uses the higher‐resolution SYM‐H in place of Dst, we are able to reveal the individual components of different solar wind‐magnetosphere interaction processes as they contribute to the geomagnetic disturbance. This is achieved with a graphics processing unit (GPU)‐based NARMAX code that is around 10 orders of magnitude faster than previous efforts from 2005, before general‐purpose programming on GPUs was possible. The algorithm includes a composite cost function, to minimize overfitting, and iterative reorthogonalization, which reduces computational errors in the most critical calculations by a factor of ∼106. The results show that negative deviations in SYM‐H following a southward interplanetary magnetic field (IMF) are first a measure of the increased magnetic flux in the geomagnetic tail, observed with a delay of 20–30 min from the time the solar wind hits the bow shock. Terms with longer delays are found which represent the dipolarization of the magnetotail, the injections of particles into the ring current, and their subsequent loss by flowout through the dayside magnetopause. Our results indicate that the contribution of magnetopause currents to the storm time indices increase with solar wind electric field, E = v × B. This is in agreement with previous studies that have shown that the magnetopause is closer to the Earth when the IMF is in the tangential direction. Key Points Empirical model of SW‐magnetosphere coupling gives insight into the various mechanisms and provides formulas to quantify their effects New GPU‐based NARMAX code is used: 1 million times more precise and 10 billion times faster than previous efforts Very small changes in SYM‐H that occur on short timescales can be accurately reproduced by the model using just solar wind data</description><identifier>ISSN: 1542-7390</identifier><identifier>ISSN: 1539-4964</identifier><identifier>EISSN: 1542-7390</identifier><identifier>DOI: 10.1002/2016SW001467</identifier><language>eng</language><publisher>Washington: John Wiley &amp; Sons, Inc</publisher><subject>Algorithms ; Charged particles ; Cost function ; Coupling ; Decoding ; Delay ; Disturbance ; Electric fields ; Fluctuations ; geomagnetic storms ; Geomagnetic tail ; Geomagnetism ; Graphics processing units ; Interplanetary magnetic field ; Interplanetary magnetic fields ; Iterative methods ; Magnetic fields ; Magnetic flux ; Magnetopause ; Magnetopause currents ; Magnetosphere ; Magnetospheres ; Magnetotails ; Mathematical models ; Nonlinearity ; numerical modeling ; Particulate composites ; Programming ; Ring currents ; Solar physics ; Solar wind ; solar wind coupling ; Solar wind-magnetosphere coupling ; Space weather ; Wind power generation</subject><ispartof>Space Weather, 2016-10, Vol.14 (10), p.724-741</ispartof><rights>2016. 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J.</creatorcontrib><creatorcontrib>Honary, F.</creatorcontrib><title>Decoding solar wind‐magnetosphere coupling</title><title>Space Weather</title><description>We employ a new NARMAX (Nonlinear Auto‐Regressive Moving Average with eXogenous inputs) code to disentangle the time‐varying relationship between the solar wind and SYM‐H. The NARMAX method has previously been used to formulate a Dst model, using a preselected solar wind coupling function. In this work, which uses the higher‐resolution SYM‐H in place of Dst, we are able to reveal the individual components of different solar wind‐magnetosphere interaction processes as they contribute to the geomagnetic disturbance. This is achieved with a graphics processing unit (GPU)‐based NARMAX code that is around 10 orders of magnitude faster than previous efforts from 2005, before general‐purpose programming on GPUs was possible. The algorithm includes a composite cost function, to minimize overfitting, and iterative reorthogonalization, which reduces computational errors in the most critical calculations by a factor of ∼106. The results show that negative deviations in SYM‐H following a southward interplanetary magnetic field (IMF) are first a measure of the increased magnetic flux in the geomagnetic tail, observed with a delay of 20–30 min from the time the solar wind hits the bow shock. Terms with longer delays are found which represent the dipolarization of the magnetotail, the injections of particles into the ring current, and their subsequent loss by flowout through the dayside magnetopause. Our results indicate that the contribution of magnetopause currents to the storm time indices increase with solar wind electric field, E = v × B. This is in agreement with previous studies that have shown that the magnetopause is closer to the Earth when the IMF is in the tangential direction. Key Points Empirical model of SW‐magnetosphere coupling gives insight into the various mechanisms and provides formulas to quantify their effects New GPU‐based NARMAX code is used: 1 million times more precise and 10 billion times faster than previous efforts Very small changes in SYM‐H that occur on short timescales can be accurately reproduced by the model using just solar wind data</description><subject>Algorithms</subject><subject>Charged particles</subject><subject>Cost function</subject><subject>Coupling</subject><subject>Decoding</subject><subject>Delay</subject><subject>Disturbance</subject><subject>Electric fields</subject><subject>Fluctuations</subject><subject>geomagnetic storms</subject><subject>Geomagnetic tail</subject><subject>Geomagnetism</subject><subject>Graphics processing units</subject><subject>Interplanetary magnetic field</subject><subject>Interplanetary magnetic fields</subject><subject>Iterative methods</subject><subject>Magnetic fields</subject><subject>Magnetic flux</subject><subject>Magnetopause</subject><subject>Magnetopause currents</subject><subject>Magnetosphere</subject><subject>Magnetospheres</subject><subject>Magnetotails</subject><subject>Mathematical models</subject><subject>Nonlinearity</subject><subject>numerical modeling</subject><subject>Particulate composites</subject><subject>Programming</subject><subject>Ring currents</subject><subject>Solar physics</subject><subject>Solar wind</subject><subject>solar wind coupling</subject><subject>Solar wind-magnetosphere coupling</subject><subject>Space weather</subject><subject>Wind power generation</subject><issn>1542-7390</issn><issn>1539-4964</issn><issn>1542-7390</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>24P</sourceid><recordid>eNqN0b9OwzAQBnALgUQpbDxAJRYGAmfnHDsjKuWPVImhoI6W415KqjQOcaOqG4_AM_IkpCpDxYCY7oaf7vTpY-ycwzUHEDcCeDKZAnBM1AHrcYkiUnEKh3v7MTsJYdFplAJ77OqOnJ8V1XwQfGmbwbqoZl8fn0s7r2jlQ_1GDQ2cb-uyM6fsKLdloLOf2Wev96OX4WM0fn54Gt6OI4fA00ihRBJJRhlyzQVl2lGc6wzQImGcO7LSgnYWcmmtRJeh4FbJLCeU2sm4zy53d-vGv7cUVmZZBEdlaSvybTBcJyil4Kj-QSWoRAuxpRe_6MK3TdUFMTwFnXKpJPypdBcshe5zp8ROrYuSNqZuiqVtNoaD2RZh9oswk-lIQJyk8TfMGXrv</recordid><startdate>201610</startdate><enddate>201610</enddate><creator>Beharrell, M. 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J.</creatorcontrib><creatorcontrib>Honary, F.</creatorcontrib><collection>Wiley Online Library Open Access</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>Space Weather</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Beharrell, M. J.</au><au>Honary, F.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Decoding solar wind‐magnetosphere coupling</atitle><jtitle>Space Weather</jtitle><date>2016-10</date><risdate>2016</risdate><volume>14</volume><issue>10</issue><spage>724</spage><epage>741</epage><pages>724-741</pages><issn>1542-7390</issn><issn>1539-4964</issn><eissn>1542-7390</eissn><abstract>We employ a new NARMAX (Nonlinear Auto‐Regressive Moving Average with eXogenous inputs) code to disentangle the time‐varying relationship between the solar wind and SYM‐H. The NARMAX method has previously been used to formulate a Dst model, using a preselected solar wind coupling function. In this work, which uses the higher‐resolution SYM‐H in place of Dst, we are able to reveal the individual components of different solar wind‐magnetosphere interaction processes as they contribute to the geomagnetic disturbance. This is achieved with a graphics processing unit (GPU)‐based NARMAX code that is around 10 orders of magnitude faster than previous efforts from 2005, before general‐purpose programming on GPUs was possible. The algorithm includes a composite cost function, to minimize overfitting, and iterative reorthogonalization, which reduces computational errors in the most critical calculations by a factor of ∼106. The results show that negative deviations in SYM‐H following a southward interplanetary magnetic field (IMF) are first a measure of the increased magnetic flux in the geomagnetic tail, observed with a delay of 20–30 min from the time the solar wind hits the bow shock. Terms with longer delays are found which represent the dipolarization of the magnetotail, the injections of particles into the ring current, and their subsequent loss by flowout through the dayside magnetopause. Our results indicate that the contribution of magnetopause currents to the storm time indices increase with solar wind electric field, E = v × B. This is in agreement with previous studies that have shown that the magnetopause is closer to the Earth when the IMF is in the tangential direction. Key Points Empirical model of SW‐magnetosphere coupling gives insight into the various mechanisms and provides formulas to quantify their effects New GPU‐based NARMAX code is used: 1 million times more precise and 10 billion times faster than previous efforts Very small changes in SYM‐H that occur on short timescales can be accurately reproduced by the model using just solar wind data</abstract><cop>Washington</cop><pub>John Wiley &amp; Sons, Inc</pub><doi>10.1002/2016SW001467</doi><tpages>18</tpages><oa>free_for_read</oa></addata></record>
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source Wiley Online Library Journals Frontfile Complete; EZB-FREE-00999 freely available EZB journals
subjects Algorithms
Charged particles
Cost function
Coupling
Decoding
Delay
Disturbance
Electric fields
Fluctuations
geomagnetic storms
Geomagnetic tail
Geomagnetism
Graphics processing units
Interplanetary magnetic field
Interplanetary magnetic fields
Iterative methods
Magnetic fields
Magnetic flux
Magnetopause
Magnetopause currents
Magnetosphere
Magnetospheres
Magnetotails
Mathematical models
Nonlinearity
numerical modeling
Particulate composites
Programming
Ring currents
Solar physics
Solar wind
solar wind coupling
Solar wind-magnetosphere coupling
Space weather
Wind power generation
title Decoding solar wind‐magnetosphere coupling
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