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dc.contributor.authorHutchinson, Ian Horner
dc.date.accessioned2015-03-04T20:51:50Z
dc.date.available2015-03-04T20:51:50Z
dc.date.issued2013-05
dc.date.submitted2013-03
dc.identifier.issn21699380
dc.identifier.issn2169-9402
dc.identifier.urihttp://hdl.handle.net/1721.1/95829
dc.description.abstractThe observation of parallel ion velocity in the near-lunar wake approximately equal to external solar wind velocity can be explained within uncertainties by an analytic electrostatic expansion model. The one-dimensional model frequently used is inadequate because it does not account for the moon's spherical shape. However, application of a more recent generalization to three dimensions of the solution along characteristics predicts higher velocities and is probably sufficient to account for the SARA observations on the Chandrayaan-1 spacecraft.en_US
dc.language.isoen_US
dc.publisherAmerican Geophysical Union (AGU)en_US
dc.relation.isversionofhttp://dx.doi.org/10.1002/jgra.50277en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourcearXiven_US
dc.titleNear-lunar proton velocity distribution explained by electrostatic accelerationen_US
dc.typeArticleen_US
dc.identifier.citationHutchinson, I. H. “Near-Lunar Proton Velocity Distribution Explained by Electrostatic Acceleration.” Journal of Geophysical Research: Space Physics 118, no. 5 (May 2013): 1825–1827.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Nuclear Science and Engineeringen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Centeren_US
dc.contributor.mitauthorHutchinson, Ian H.en_US
dc.relation.journalJournal of Geophysical Research: Space Physicsen_US
dc.eprint.versionOriginal manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/NonPeerRevieweden_US
dspace.orderedauthorsHutchinson, I. H.en_US
mit.licenseOPEN_ACCESS_POLICYen_US
mit.metadata.statusComplete


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