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dc.contributor.authorArcher, M. O.
dc.contributor.authorSouthwood, D. J.
dc.contributor.authorHartinger, M. D.
dc.contributor.authorRastaetter, L.
dc.contributor.authorWright, A. N.
dc.date.accessioned2022-02-08T17:30:01Z
dc.date.available2022-02-08T17:30:01Z
dc.date.issued2022-02
dc.identifier277692514
dc.identifier7c1c4b68-b9b7-4f1c-a5bd-85ec55e66182
dc.identifier85125413659
dc.identifier000765721800045
dc.identifier.citationArcher , M O , Southwood , D J , Hartinger , M D , Rastaetter , L & Wright , A N 2022 , ' How a realistic magnetosphere alters the polarizations of surface, fast magnetosonic, and Alfvén waves ' , Journal of Geophysical Research: Space Physics , vol. 127 , no. 2 , e2021JA030032 . https://doi.org/10.1029/2021JA030032en
dc.identifier.issn2169-9380
dc.identifier.otherRIS: urn:A954427144DDE77C59CEC8BA666589B8
dc.identifier.otherORCID: /0000-0002-9877-1457/work/108118658
dc.identifier.urihttps://hdl.handle.net/10023/24827
dc.descriptionFunding: MOA holds a UKRI (STFC / EPSRC) Stephen Hawking Fellowship EP/T01735X/1. DJS was supported by STFC grant ST/S000364/1. MDH was supported by NASA grant 80NSSC19K0127. A.N.W. was partially funded by STFC grant ST/N000609/1.en
dc.description.abstractSystem-scale magnetohydrodynamic (MHD) waves within Earth?s magnetosphere are often understood theoretically using box models. While these have been highly instructive in understanding many fundamental features of the various wave modes present, they neglect the complexities of geospace such as the inhomogeneities and curvilinear geometries present. Here we show global MHD simulations of resonant waves impulsively-excited by a solar wind pressure pulse. Although many aspects of the surface, fast magnetosonic (cavity/waveguide), and Alfvén modes present agree with the box and axially symmetric dipole models, we find some predictions for large-scale waves are significantly altered in a realistic magnetosphere. The radial ordering of fast mode turning points and Alfvén resonant locations may be reversed even with monotonic wave speeds. Additional nodes along field lines that are not present in the displacement/velocity occur in both the perpendicular and compressional components of the magnetic field. Close to the magnetopause the perpendicular oscillations of the magnetic field have the opposite handedness to the velocity. Finally, widely-used detection techniques for standing waves, both across and along the field, can fail to identify their presence. We explain how all these features arise from the MHD equations when accounting for a non-uniform background field and propose modified methods which might be applied to spacecraft observations.
dc.format.extent23
dc.format.extent8597218
dc.language.isoeng
dc.relation.ispartofJournal of Geophysical Research: Space Physicsen
dc.subjectUlf wavesen
dc.subjectPolarizationen
dc.subjectMagnetohydrodynamicsen
dc.subjectSimulationen
dc.subjectTheoryen
dc.subjectQA Mathematicsen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectDASen
dc.subject.lccQAen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleHow a realistic magnetosphere alters the polarizations of surface, fast magnetosonic, and Alfvén wavesen
dc.typeJournal articleen
dc.contributor.sponsorScience & Technology Facilities Councilen
dc.contributor.institutionUniversity of St Andrews. Applied Mathematicsen
dc.identifier.doihttps://doi.org/10.1029/2021JA030032
dc.description.statusPeer revieweden
dc.identifier.grantnumberST/N000609/1en


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