Magnetic holes in the solar wind between 0.3 AU and 17 AU

dc.bibliographicCitation.firstPage191eng
dc.bibliographicCitation.issue3-4eng
dc.bibliographicCitation.volume7eng
dc.contributor.authorSperveslage, K.
dc.contributor.authorNeubauer, F.M.
dc.contributor.authorBaumgärtel, K.
dc.contributor.authorNess, N.F.
dc.date.accessioned2020-08-07T13:48:32Z
dc.date.available2020-08-07T13:48:32Z
dc.date.issued2000
dc.description.abstractMagnetic holes (MHs) are depressions of the magnetic field magnitude. Turner et al. (1977) identified the first MHs in the solar wind and determined an occurrence rate of 1.5 MHs/d. Winterhalter et al. (1994) developed an automatic identification criterion to search for MHs in Ulysses data in the solar wind between 1 AU and 5.4 AU. We adopt their criterion to expand the search to the heliocentric distances down to 0.3 AU using data from Helios 1 and 2 and up to 17 AU using data from Voyager 2. We relate our observations to two theoretical approaches which describe the so-called linear MHs in which the magnetic vector varies in magnitude rather than direction. Therefore we focus on such linear MHs with a directional change less than 10°. With our observations of about 850 MHs we present the following results: Approximately 30% of all the identified MHs are linear. The maximum angle between the initial magnetic field vector and any vector inside the MH is 20°in average and shows a weak relation to the depth of the MHs. The angle between the initial magnetic field and the minimum variance direction of those structures is large and very probably close to 90°. The MHs are placed in a high β environment even though the average solar wind shows a smaller β. The widths decrease from about 50 proton inertial length in a region between 0.3 AU and 0.4 AU heliocentric distance to about 15 proton inertial length at distances larger than 10 AU. This quantity is correlated with the β of the MH environments with respect to the heliocentric distance. There is a clear preference for the occurrence of depressions instead of compressions. We discuss these results with regard to the main theories of MHs, the mirror instability and the alternative soliton approach. Although our observational results are more consistent with the soliton theory we favor a combination of both. MHs might be the remnants of initial mirror mode structures which can be described as solitons during the main part of their lifetime.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://doi.org/10.34657/4039
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/5410
dc.language.isoengeng
dc.publisherGöttingen : Copernicus GmbHeng
dc.relation.doihttps://doi.org/10.5194/npg-7-191-2000
dc.relation.ispartofseriesNonlinear Processes in Geophysics 7 (2000), Nr. 3-4eng
dc.relation.issn1023-5809
dc.rights.licenseCC BY-NC-SA 2.5 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by-nc-sa/2.5/eng
dc.subjectsolar windeng
dc.subject.ddc530eng
dc.titleMagnetic holes in the solar wind between 0.3 AU and 17 AUeng
dc.typearticleeng
dc.typeTexteng
dcterms.bibliographicCitation.journalTitleNonlinear Processes in Geophysicseng
tib.accessRightsopenAccesseng
wgl.contributorAIPeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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