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Empirical modeling of the geomagnetosphere for SIR and CME-driven magnetic storms. / Andreeva, V.A.; Tsyganenko, N.A. .

In: JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS, Vol. 124, No. 7, 01.01.2019, p. 5641-5662.

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Andreeva, V.A. ; Tsyganenko, N.A. . / Empirical modeling of the geomagnetosphere for SIR and CME-driven magnetic storms. In: JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS. 2019 ; Vol. 124, No. 7. pp. 5641-5662.

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@article{8a854f5253864a528b768e746fe20c96,
title = "Empirical modeling of the geomagnetosphere for SIR and CME-driven magnetic storms",
abstract = "During geomagnetic disturbances, the solar wind arrives in the form of characteristic sequences lasting from tens of hours to days. The most important magnetic storm drivers are the coronal mass ejections (CMEs) and the slow-fast stream interaction regions (SIRs). Previous data-based magnetic field models did not distinguish between these types of the solar wind driving. In the present work we retained the basic structure of the Tsyganenko and Andreeva (2015) model but fitted it to data samples corresponding to (1) SIR-driven storms, (2) CME-driven storms preceded with a shock ahead of the CME, and (3) CME-driven storms without such shocks. The storm time dynamics of the model current systems has been represented using the parametrization method developed by Tsyganenko and Sitnov (2005), based on dynamical variables W i, calculated from concurrent solar wind characteristics and their previous history. The database included observations of THEMIS, Polar, Cluster, Geotail, and Van Allen Probes missions during 155 storms in 1997–2016. The model current systems drastically differ from each other with respect to decay rate and total current magnitudes. During SIR-induced storms, all current systems saturate, while during CME-induced disturbances, the saturation occurs only for the symmetric ring current and the tail current. The partial ring current parameters are drastically different between SIR- and CME-induced storm sets. In the case of SIR-driven storms, the total partial ring current is comparable with symmetric ring current, whereas for all CME-induced events it is nearly twice higher. The results are compared with GOES 15 magnetometer observations. ",
keywords = "magnetic storms, magnetosphere, modeling, solar wind, spacecraft data, DST, INTERPLANETARY CONDITIONS, FIELD, SOLAR-WIND, QUIET, MAGNETOSPHERE, CIR",
author = "V.A. Andreeva and N.A. Tsyganenko",
year = "2019",
month = jan,
day = "1",
doi = "https://doi. org/10.1029/2018JA026008",
language = "English",
volume = "124",
pages = "5641--5662",
journal = "Journal of Geophysical Research: Biogeosciences",
issn = "0148-0227",
publisher = "American Geophysical Union",
number = "7",

}

RIS

TY - JOUR

T1 - Empirical modeling of the geomagnetosphere for SIR and CME-driven magnetic storms

AU - Andreeva, V.A.

AU - Tsyganenko, N.A.

PY - 2019/1/1

Y1 - 2019/1/1

N2 - During geomagnetic disturbances, the solar wind arrives in the form of characteristic sequences lasting from tens of hours to days. The most important magnetic storm drivers are the coronal mass ejections (CMEs) and the slow-fast stream interaction regions (SIRs). Previous data-based magnetic field models did not distinguish between these types of the solar wind driving. In the present work we retained the basic structure of the Tsyganenko and Andreeva (2015) model but fitted it to data samples corresponding to (1) SIR-driven storms, (2) CME-driven storms preceded with a shock ahead of the CME, and (3) CME-driven storms without such shocks. The storm time dynamics of the model current systems has been represented using the parametrization method developed by Tsyganenko and Sitnov (2005), based on dynamical variables W i, calculated from concurrent solar wind characteristics and their previous history. The database included observations of THEMIS, Polar, Cluster, Geotail, and Van Allen Probes missions during 155 storms in 1997–2016. The model current systems drastically differ from each other with respect to decay rate and total current magnitudes. During SIR-induced storms, all current systems saturate, while during CME-induced disturbances, the saturation occurs only for the symmetric ring current and the tail current. The partial ring current parameters are drastically different between SIR- and CME-induced storm sets. In the case of SIR-driven storms, the total partial ring current is comparable with symmetric ring current, whereas for all CME-induced events it is nearly twice higher. The results are compared with GOES 15 magnetometer observations.

AB - During geomagnetic disturbances, the solar wind arrives in the form of characteristic sequences lasting from tens of hours to days. The most important magnetic storm drivers are the coronal mass ejections (CMEs) and the slow-fast stream interaction regions (SIRs). Previous data-based magnetic field models did not distinguish between these types of the solar wind driving. In the present work we retained the basic structure of the Tsyganenko and Andreeva (2015) model but fitted it to data samples corresponding to (1) SIR-driven storms, (2) CME-driven storms preceded with a shock ahead of the CME, and (3) CME-driven storms without such shocks. The storm time dynamics of the model current systems has been represented using the parametrization method developed by Tsyganenko and Sitnov (2005), based on dynamical variables W i, calculated from concurrent solar wind characteristics and their previous history. The database included observations of THEMIS, Polar, Cluster, Geotail, and Van Allen Probes missions during 155 storms in 1997–2016. The model current systems drastically differ from each other with respect to decay rate and total current magnitudes. During SIR-induced storms, all current systems saturate, while during CME-induced disturbances, the saturation occurs only for the symmetric ring current and the tail current. The partial ring current parameters are drastically different between SIR- and CME-induced storm sets. In the case of SIR-driven storms, the total partial ring current is comparable with symmetric ring current, whereas for all CME-induced events it is nearly twice higher. The results are compared with GOES 15 magnetometer observations.

KW - magnetic storms

KW - magnetosphere

KW - modeling

KW - solar wind

KW - spacecraft data

KW - DST

KW - INTERPLANETARY CONDITIONS

KW - FIELD

KW - SOLAR-WIND

KW - QUIET

KW - MAGNETOSPHERE

KW - CIR

UR - http://www.scopus.com/inward/record.url?scp=85071068778&partnerID=8YFLogxK

UR - http://www.mendeley.com/research/empirical-modeling-geomagnetosphere-sir-cmedriven-magnetic-storms

U2 - https://doi. org/10.1029/2018JA026008

DO - https://doi. org/10.1029/2018JA026008

M3 - Article

VL - 124

SP - 5641

EP - 5662

JO - Journal of Geophysical Research: Biogeosciences

JF - Journal of Geophysical Research: Biogeosciences

SN - 0148-0227

IS - 7

ER -

ID: 45304648