{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1362544419956278528.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1029/94ja00142"}},{"identifier":{"@type":"URI","@value":"https://api.wiley.com/onlinelibrary/tdm/v1/articles/10.1029%2F94JA00142"}},{"identifier":{"@type":"URI","@value":"https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/94JA00142"}}],"dc:title":[{"@value":"Numerical simulation of torus‐driven plasma transport in the Jovian magnetosphere"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>The Rice convection model has been modified for application to the transport of Io‐generated plasma through the Jovian magnetosphere. The new code, called the RCM‐J, has been used for several ideal‐MHD numerical simulations to study how interchange instability causes an initially assumed torus configuration to break up. In simulations that start from a realistic torus configuration but include no energetic particles, the torus disintegrates too quickly (∼50 hours). By adding an impounding distribution of energetic particles to suppress the interchange instability, reasonable lifetimes were obtained. For cases in which impoundment is insufficient to produce ideal‐MHD stability, the torus breaks up predominantly into long fingers, unless the initial condition strongly favors some other geometrical form. If the initial torus has more mass on one side of the planet than the other, fingers form predominantly on the heavy side (which we associate with the active sector). Coriolis force bends the fingers to lag corotation. The simulation results are consistent with the idea that the fingers are formed with a longitudinal thickness that is roughly equal to the latitudinal distance over which the invariant density declines at the outer edges of the initial torus. Our calculations give an average longitudinal distance between plasma fingers of about 15°, which corresponds to 20 to 30 minutes of rotation of the torus. We point to some Voyager and Ulysses data that are consistent with this scale of torus longitudinal irregularity.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380306905150273048","@type":"Researcher","foaf:name":[{"@value":"Y. S. Yang"}]},{"@id":"https://cir.nii.ac.jp/crid/1382544419956278530","@type":"Researcher","foaf:name":[{"@value":"R. A. Wolf"}]},{"@id":"https://cir.nii.ac.jp/crid/1382544419956278528","@type":"Researcher","foaf:name":[{"@value":"R. W. Spiro"}]},{"@id":"https://cir.nii.ac.jp/crid/1382544419956278531","@type":"Researcher","foaf:name":[{"@value":"T. W. Hill"}]},{"@id":"https://cir.nii.ac.jp/crid/1382544419956278532","@type":"Researcher","foaf:name":[{"@value":"A. J. Dessler"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"01480227"}],"prism:publicationName":[{"@value":"Journal of Geophysical Research: Space Physics"}],"dc:publisher":[{"@value":"American Geophysical Union (AGU)"}],"prism:publicationDate":"1994-05","prism:volume":"99","prism:number":"A5","prism:startingPage":"8755","prism:endingPage":"8770"},"reviewed":"false","dc:rights":["http://onlinelibrary.wiley.com/termsAndConditions#vor"],"url":[{"@id":"https://api.wiley.com/onlinelibrary/tdm/v1/articles/10.1029%2F94JA00142"},{"@id":"https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1029/94JA00142"}],"createdAt":"2004-02-03","modifiedAt":"2023-09-23","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001202716094592","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Response of Jupiter's Aurora to Plasma Mass Loading Rate Monitored by the Hisaki Satellite During Volcanic Eruptions at Io"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306905150272512","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Mass Supply from Io to Jupiter’s Magnetosphere"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846641064845568","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Io torus plasma transport under interchange instability and flow shears"}]},{"@id":"https://cir.nii.ac.jp/crid/2051714791980358528","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Volcanic activity on Io and its influence on the dynamics of the Jovian magnetosphere observed by EXCEED/Hisaki in 2015"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1029/94ja00142"},{"@type":"CROSSREF","@value":"10.1002/2017ja025029_references_DOI_YTUvIsZwhezYhWfNOCpgWu4SfXt"},{"@type":"CROSSREF","@value":"10.1016/j.pss.2011.11.014_references_DOI_YTUvIsZwhezYhWfNOCpgWu4SfXt"},{"@type":"CROSSREF","@value":"10.1007/s11214-025-01137-x_references_DOI_YTUvIsZwhezYhWfNOCpgWu4SfXt"},{"@type":"CROSSREF","@value":"10.1186/s40623-017-0700-9_references_DOI_YTUvIsZwhezYhWfNOCpgWu4SfXt"}]}