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The spatial distribution of water in the inner coma of Comet 9P/Tempel 1: Comparison between models and observations

dc.citation.epage23en_US
dc.citation.issueen_US
dc.citation.spage9en_US
dc.citation.volume236en_US
dc.citation.woscount1
dc.contributor.authorFinklenburg, S.en_US
dc.contributor.authorThomas, N.en_US
dc.contributor.authorSu, C. C.en_US
dc.contributor.authorWu, J. -S.en_US
dc.contributor.department機械工程學系zh_TW
dc.contributor.departmentDepartment of Mechanical Engineeringen_US
dc.date.accessioned2014-12-08T15:36:02Z
dc.date.available2014-12-08T15:36:02Z
dc.date.issued2014-07-01en_US
dc.description.abstractThe near nucleus coma of Comet 9P/Tempel 1 has been simulated with the 3D Direct Simulation Monte Carlo (DSMC) code PDSC++ (Su, C.-C. [2013]. Parallel Direct Simulation Monte Carlo (DSMC) Methods for Modeling Rarefied Gas Dynamics. PhD Thesis, National Chiao Tung University, Taiwan) and the derived column densities have been compared to observations of the water vapour distribution found by using infrared imaging spectrometer on the Deep Impact spacecraft (Feaga, L.M., A\'Hearn, M.F., Sunshine, J.M., Groussin, O., Farnham, T.L. [2007]. Icarus 191(2), 134-145. http://dx.doi.org/10.1016/j.icarus.2007.04.038). Modelled total production rates are also compared to various observations made at the time of the Deep Impact encounter. Three different models were tested. For all models, the shape model constructed from the Deep Impact observations by Thomas et al. (Thomas, P.C., Veverka, J., Belton, M.J.S., Hidy, A., A\'Hearn, M.F., Farnham, T.L., et al. [2007]. Icarus, 187(1), 4-15. http://dx.doi.org/10.1016/j.icarus.2006.12.013) was used. Outgassing depending only on the cosine of the solar insolation angle on each shape model facet is shown to provide an unsatisfactory model. Models constructed on the basis of active areas suggested by Kossacki and Szutowicz (Kossacki, K, Szutowicz, S. [2008]. Icarus, 195(2), 705-724. http://dx.doi.org/ 10.1016/j.icarus.2007.12.014) are shown to be superior. The Kossacki and Szutowicz model, however, also shows deficits which we have sought to improve upon. For the best model we investigate the properties of the outflow. (C) 2014 Elsevier Inc. All rights reserved.en_US
dc.identifier.doi10.1016/j.icarus.2014.03.032en_US
dc.identifier.issn0019-1035en_US
dc.identifier.journalICARUSen_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.icarus.2014.03.032en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/24393
dc.identifier.wosnumberWOS:000336477400002
dc.language.isoen_USen_US
dc.subjectComet Tempel 1en_US
dc.subjectComet, comaen_US
dc.subjectComets, nucleusen_US
dc.titleThe spatial distribution of water in the inner coma of Comet 9P/Tempel 1: Comparison between models and observationsen_US
dc.typeArticleen_US

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