Lunar Plasma Environment in Magnetotail Lobe Conditions. First Results from 3-D Hybrid Kinetic Modeling and Comparison with ARTEMIS Observation

dc.contributor.authorLipatov, Alexander
dc.contributor.authorHalekas, Jasper S.
dc.contributor.authorSarantos, Menelaos
dc.contributor.authorCooper, John F.
dc.date.accessioned2022-08-17T14:47:28Z
dc.date.available2022-08-17T14:47:28Z
dc.date.issued2022-02-25
dc.descriptionAGU 2021 Fall Meeting, 13-17 December 2021, New Orleans, LA and virtualen_US
dc.description.abstractThe study of lunar plasma environment's response to the magnetotail lobe condition is the main subject of our investigation in this report. Photoionization and charge exchange of protons with the lunar exosphere arethe ionization processes included in our model. The computational model includes the dynamics of heavy Na+ pickup and ambient magnetospheric ions. The electrons are considered as a fluid.The lunar interior is considered as a weakly conducting body. In this report we consider for the first time a formation of lunar plasma structures, wakes, and a generation of low-frequency electromagnetic waves by using a self-consistent hybrid kinetic modeling. The input parameters were taken from the ARTEMIS observations. At an early stage the Moon with exosphere and conducting core excites whistler waves in case of Sub-Alfvenic/sonic interaction. At a later stage an excitation of the Alfven wave is observed. The topology of the Alfven waves is approximately similar to the Alfven wing near the planetary moons (Io, Europa etc.). The physics of the Moon-magnetotail lobe interaction is also close to the physics of the interaction between plasma clouds (expanding and not expanding) and ambient magnetospheric plasma. The heavy pickup ions create a large structured halo with space scale of more than 10 R_{E} in the direction of the background field. The modeling also shows an excitation of the compressional waves due to expansion of heavy exospheric pickup ions. The lunar model with weaker interior conductivity excites lower levels of the wave activity.en_US
dc.description.sponsorshipThis work was supported by NASA Award (80NSSC20K0146) from Solar System Workings Program (NNH18ZDA001N-C.3-SSW2018). Computational resources were provided by the NASA High-End SupercomputingFacilities (Aitken-Ames, Project HEC SMD-20-02357875).en_US
dc.description.urihttps://www.essoar.org/doi/10.1002/essoar.10510591.1en_US
dc.format.extent10 pagesen_US
dc.genrepresentations (communicative events)en_US
dc.genreconference papers and proceedingsen_US
dc.identifierdoi:10.13016/m2isi5-1kxm
dc.identifier.urihttps://doi.org/10.1002/essoar.10510591.1
dc.identifier.urihttp://hdl.handle.net/11603/25418
dc.language.isoen_USen_US
dc.relation.isAvailableAtThe University of Maryland, Baltimore County (UMBC)
dc.relation.ispartofUMBC Goddard Planetary Heliophysics Institute (GPHI)
dc.relation.ispartofUMBC Faculty Collection
dc.rightsThis work was written as part of one of the author's official duties as an Employee of the United States Government and is therefore a work of the United States Government. In accordance with 17 U.S.C. 105, no copyright protection is available for such works under U.S. Law.en_US
dc.rightsPublic Domain Mark 1.0*
dc.rights.urihttp://creativecommons.org/publicdomain/mark/1.0/*
dc.titleLunar Plasma Environment in Magnetotail Lobe Conditions. First Results from 3-D Hybrid Kinetic Modeling and Comparison with ARTEMIS Observationen_US
dc.typeTexten_US
dcterms.creatorhttps://orcid.org/0000-0001-5026-8214en_US

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