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Origin of interplanetary southward magnetic fields responsible for major magnetic storms near solar maximum (1978–1979)
627
Citations
44
References
1988
Year
EngineeringSheath FieldsSolar ConvectionPlasma PhysicsSolar-terrestrial InteractionSolar PhysicGeophysicsGeospace PhysicsSolar Terrestrial EnvironmentCosmic PlasmaPlasma TheoryMagnetohydrodynamicsSpace PhysicPlanetary MagnetosphereSolar ActivityMajor Magnetic StormsGeomagnetismAe IndexSpace WeatherMagnetospheric PlasmaAstrophysicsSolar VariabilityMagnetospheric PhysicsSolar MaximumB Z Event
The origins of the interplanetary southward B z which cause the 10 major ( D st < −100 nT) magnetic storms detected during the 500 days of study (August 16, 1978, to December 28, 1979) of the Gonzalez and Tsurutani (1987) work are examined in detail. A full complement of ISEE 3 plasma and field data, an 11‐station AE index and the near‐equatorial D st index, are used in this analysis. It is found that the origins of the interplanetary southward B z events are quite varied. If it is defined that the B z event which leads to D st < −100 nT is “the cause” of the storm, then one of the storm intensifications is caused by shock compression of preexisting southward interplanetary magnetic fields, four (or five) are related to driver gas magnetic fields, one (or two) are caused by shocked kinky heliospheric current sheets, two (or three) by turbulence or waves behind interplanetary shocks, and one possibly by draped fields associated with a noncompressive density enhancement event (without a shock or a high‐speed stream). In simplistic terms, four (or five) storms are caused by driver gas fields, four by shocked (sheath) fields, and one possibly by high‐intensity draped fields. In actuality, many of the interplanetary southward B z and corresponding magnetic storm ( D st ) structures are more complex than stated above. At least four of the interplanetary events have both major sheath and driver gas southward B z events. In two storms, sheath southward B z features led to D st reaching levels of −90 nT prior to driver gas southward B z features; the following driver gas fields then caused D st to exceed our storm criteria of ≤ −100 nT. In two other cases, sheath B z features led to magnetic storm onsets ( D st < −100 nT); the following driver gas southward B z features cause further storm intensifications. The above magnetic storms therefore displayed two‐stage development characteristics. The results of this study indicate the equal importance of both sheath fields or draped fields and driver gas fields for the generation of major geomagnetic storms. Because of the importance of the sheath fields the intensity and duration of geomagnetic storms cannot be predicted by solar observations of active regions alone. Tang et al. (1988) will address this topic in detail.
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