{"@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/1360004232184474752.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/j.icarus.2018.02.027"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0019103517308023?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0019103517308023?httpAccept=text/plain"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Thermal conductivity of lunar regolith simulant JSC-1A under vacuum"}],"description":[{"notation":[{"@value":"Abstract   Many air-less planetary bodies, including the Moon, asteroids, and comets, are covered by regolith. The thermal conductivity of the regolith is an essential parameter controlling the surface temperature variation. A thermal conductivity model applicable to natural soils as well as planetary surface regolith is required to analyze infrared remote sensing data. In this study, we investigated the temperature and compressional stress dependence of the thermal conductivity of the lunar regolith simulant JSC-1A, and the temperature dependence of sieved JSC-1A samples under vacuum conditions. We confirmed that a series of the experimental data for JSC-1A are fitted well by our analytical model of the thermal conductivity (Sakatani et al., 2017). Comparison with the calibration data of the sieved samples with those for original JSC-1A indicates that the thermal conductivity of natural samples with a wide grain size distribution can be modeled as mono-sized grains with a volumetric median size. The calibrated model can be used to estimate the volumetric median grain size from infrared remote sensing data. Our experiments and the calibrated model indicates that uncompressed JSC-1A has similar thermal conductivity to lunar top-surface materials, but the lunar subsurface thermal conductivity cannot be explained only by the effects of the density and self-weighted compressional stress. We infer that the nature of the lunar subsurface regolith grains is much different from JSC-1A and lunar top-surface regolith, and/or the lunar subsurface regolith is over-consolidated and the compressional stress higher than the hydrostatic pressure is stored in the lunar regolith layer."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004232184474754","@type":"Researcher","foaf:name":[{"@value":"Naoya Sakatani"}]},{"@id":"https://cir.nii.ac.jp/crid/1380004232184474755","@type":"Researcher","foaf:name":[{"@value":"Kazunori Ogawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1030003658349159047","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"10222738"},{"@type":"NRID","@value":"1000010222738"},{"@type":"ORCID","@value":"0000-0003-3670-2699"},{"@type":"NRID","@value":"9000004613754"},{"@type":"NRID","@value":"9000239609448"},{"@type":"NRID","@value":"9000408632382"},{"@type":"NRID","@value":"9000250471791"},{"@type":"NRID","@value":"9000258560933"},{"@type":"NRID","@value":"9000332222968"},{"@type":"NRID","@value":"9000258560482"},{"@type":"NRID","@value":"9000408856269"},{"@type":"NRID","@value":"9000258569558"},{"@type":"NRID","@value":"9000258570363"},{"@type":"NRID","@value":"9000258560349"},{"@type":"NRID","@value":"9000367407273"},{"@type":"NRID","@value":"9000239609429"},{"@type":"NRID","@value":"9000283742040"},{"@type":"NRID","@value":"9000412299467"},{"@type":"NRID","@value":"9000412299462"},{"@type":"NRID","@value":"9000412334335"},{"@type":"NRID","@value":"9000412334330"},{"@type":"NRID","@value":"9000408829516"},{"@type":"NRID","@value":"9000408829520"},{"@type":"NRID","@value":"9000283741927"},{"@type":"NRID","@value":"9000258560327"},{"@type":"NRID","@value":"9000258559857"},{"@type":"NRID","@value":"9000243767581"},{"@type":"NRID","@value":"9000263032777"},{"@type":"NRID","@value":"9000275831882"},{"@type":"NRID","@value":"9000016886772"},{"@type":"NRID","@value":"9000283742229"},{"@type":"NRID","@value":"9000283742647"},{"@type":"NRID","@value":"9000258559859"},{"@type":"NRID","@value":"9000004602049"},{"@type":"NRID","@value":"9000283724358"},{"@type":"NRID","@value":"9000283724359"},{"@type":"NRID","@value":"9000258560454"},{"@type":"NRID","@value":"9000239848024"},{"@type":"NRID","@value":"9000412568888"},{"@type":"NRID","@value":"9000258560822"},{"@type":"NRID","@value":"9000239609479"},{"@type":"NRID","@value":"9000408632388"},{"@type":"NRID","@value":"9000258560815"},{"@type":"NRID","@value":"9000024265848"},{"@type":"NRID","@value":"9000024265859"},{"@type":"NRID","@value":"9000020054173"},{"@type":"NRID","@value":"9000258560330"},{"@type":"NRID","@value":"9000016882578"},{"@type":"NRID","@value":"9000391796438"},{"@type":"NRID","@value":"9000258559873"},{"@type":"NRID","@value":"9000254585870"},{"@type":"NRID","@value":"9000239609453"},{"@type":"NRID","@value":"9000239609412"},{"@type":"NRID","@value":"9000283742227"},{"@type":"NRID","@value":"9000258560808"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/masahiko_arakawa"}],"foaf:name":[{"@value":"Masahiko Arakawa"}]},{"@id":"https://cir.nii.ac.jp/crid/1380004232184474753","@type":"Researcher","foaf:name":[{"@value":"Satoshi Tanaka"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00191035"}],"prism:publicationName":[{"@value":"Icarus"}],"dc:publisher":[{"@value":"Elsevier 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