Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/61597
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dc.contributorDepartment of Land Surveying and Geo-Informatics-
dc.creatorChen, T-
dc.creatorShen, Y-
dc.creatorChen, Q-
dc.date.accessioned2016-12-19T08:56:30Z-
dc.date.available2016-12-19T08:56:30Z-
dc.identifier.urihttp://hdl.handle.net/10397/61597-
dc.language.isoenen_US
dc.publisherMolecular Diversity Preservation International (MDPI)en_US
dc.rights© 2016 by the authors; licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC-BY) license (http://creativecommons.org/licenses/by/4.0/).en_US
dc.rightsThe following publication Chen, T.; Shen, Y.; Chen, Q. Mass Flux Solution in the Tibetan Plateau Using Mascon Modeling. Remote Sens. 2016, 8, 439,1-17 is available at https://dx.doi.org/10.3390/rs8050439en_US
dc.subjectGRACEen_US
dc.subjectMasconen_US
dc.subjectMass flux solutionen_US
dc.subjectTibetan Plateauen_US
dc.titleMass flux solution in the Tibetan Plateau using mascon modelingen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1en_US
dc.identifier.epage17en_US
dc.identifier.volume8en_US
dc.identifier.issue5en_US
dc.identifier.doi10.3390/rs8050439en_US
dcterms.abstractMascon modeling is used in this paper to produce the mass flux solutions in the Tibetan Plateau. In the mascon modeling, the pseudo observations and their covariance matrices are derived from the GRACE monthly gravity field models. The sampling density of the pseudo observations is determined based on the eigenvalues of the covariance matrices. In the Tibetan Plateau, the sampling density of per 1.5° is the most appropriate among all choices. The mass flux variations from 2003 to 2014 are presented in this paper, which show large mass loss (about -15.5 Gt/year) in Tianshan, North India, and Eastern Himalaya, as well as strong positive signals (about 9 Gt/year) in the Inner Tibetan Plateau. After the glacier isostatic adjustment effects from Pau-5-AUT model are removed, the mass change rates in the Tibetan Plateau derived from CSR RL05, JPL RL05, GFZ RL05a, and Tongji-GRACE02 monthly models are -6.41 ± 4.74 Gt/year, -5.87 ± 4.88 Gt/year, -6.08 ± 4.65 Gt/year, and -11.50 ± 4.79 Gt/year, respectively, which indicate slight mass loss in this area. Our results confirm that mascon modeling is efficient in the recovery of time-variable gravity signals in the Tibetan Plateau.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationRemote sensing, June 2016, v. 8, no. 5, 439, p. 1-17-
dcterms.isPartOfRemote sensing-
dcterms.issued2016-
dc.identifier.isiWOS:000378406400083-
dc.identifier.scopus2-s2.0-84971477331-
dc.identifier.eissn2072-4292en_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_IR/PIRAen_US
dc.description.pubStatusPublisheden_US
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