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dc.contributor.authorBayati, MS
dc.contributor.authorKeshtkar, A
dc.contributor.authorKeshtkar, A
dc.date.accessioned2018-08-26T08:09:10Z
dc.date.available2018-08-26T08:09:10Z
dc.date.issued2011
dc.identifier.urihttp://dspace.tbzmed.ac.ir:8080/xmlui/handle/123456789/50418
dc.description.abstractThermal energy in railgun is unwanted and generated by ohmic losses that are dependent to the current implied, rail dimensions, electrical conductivity (sigma), and specific heat (C(P)). sigma and C(P) are functions of temperature. Using achievement L' formula by intelligent estimation method, the current density and ohmic losses on the cross section of the rail are computed. Ohmic losses are the source heat and utilized heat equation that are used to compute thermal distribution and temperature that are compared with other results in some papers. This paper chose h = 30 mm, w = 10 mm, and copper for the rail material and a method to compute the thermal distribution on the surface of the rail and side rail edges. Effects of rail dimensions on the temperature in time domain are calculated and shown in the figures. Rail materials are investigated with copper and aluminum in which the average temperature of both materials on the rail surface is calculated and compared.
dc.language.isoEnglish
dc.relation.ispartofIEEE TRANSACTIONS ON PLASMA SCIENCE
dc.relation.ispartof15th International Symposium on Electromagnetic Launch (EML) Technology
dc.subjectIntelligent estimation method with time variations (IEM-TD)
dc.subjectmaximum temperature
dc.subjectohmic loss
dc.subjectrailgun
dc.subjectthermal distribution
dc.titleThermal Computation in Railgun by Hybrid Time Domain Technique 3-D-FEM-IEM
dc.typeArticle; Proceedings Paper
dc.citation.volume39
dc.citation.issue1
dc.citation.spage18
dc.citation.epage21
dc.citation.indexWeb of science
dc.identifier.DOIhttps://doi.org/10.1109/TPS.2010.2070847


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