博碩士論文 100623023 完整後設資料紀錄

DC 欄位 語言
DC.contributor太空科學研究所zh_TW
DC.creator劉晉銘zh_TW
DC.creatorChin-Min Liuen_US
dc.date.accessioned2013-7-29T07:39:07Z
dc.date.available2013-7-29T07:39:07Z
dc.date.issued2013
dc.identifier.urihttp://ir.lib.ncu.edu.tw:88/thesis/view_etd.asp?URN=100623023
dc.contributor.department太空科學研究所zh_TW
DC.description國立中央大學zh_TW
DC.descriptionNational Central Universityen_US
dc.description.abstract我的論文研究主要目標在於探討及研究土星環鄰近地區之中帶著大範圍Q/m值的帶電塵埃粒子之運動軌道的演化及其物理意涵,並且藉由帶電塵埃粒子的軌道運動,其數量密度分佈亦可透過數值模擬得之。在此次的研究之中,我使用了4 階Runge-Kutta法來模擬帶電塵埃粒子之運動軌道以及使用上述之方法加上來自於Monte Carlo法的相關概念來模擬帶電塵埃粒子之數量密度分佈,並且在所有的運動軌道之中,帶電塵埃粒子的電荷值都固定不變,並且我也計算帶電塵埃粒子受到shadow effect影響之下的運動軌道及其數量密度分佈,因受到shadow effect的影響,帶電塵埃粒子之電性將會有所變化而非固定不變。根據模擬的結果顯示,當帶電塵埃粒子的Q/m≥10^-4 e/mP且出發點在穩定臨界半徑(rc=1.53 RS)內則他們將會透過虹吸式流動撞擊到土星的上層大氣,此外,土星赤道電離層減損效應也有可能是因為帶有Q/m=10^-6–10^-7 e/mP的帶電塵埃粒子入射到土星赤道上層大氣因而造成,其現象亦被Cassini太空船觀測到。假如帶電塵埃粒子受到shadow effect的影響,其運動軌道將會和單純只帶有正電荷或是負電荷之帶電塵埃粒子有很大的不同。從帶電塵埃粒子在Encke Gap內的運動軌道計算之中,我們可以瞭解到Q/m和角速度之間的關係,其可以提供軌道穩定性的相關資訊。然而,因為目前尚未有靠近土星環鄰近地區的現地量測,因此這份研究將可以提供在未來觀測時所需之模型基礎,並且亦可以解釋在土星上層大氣及土星環系統所觀測到的現象,此外,亦可解釋土星環和土星彼此之間的交互作用。zh_TW
dc.description.abstractThe objective of my thesis research aims to study the evolution and physical implications of the orbital motion of charged dust grains with different charge-to-mass ratios (Q/m) in the vicinity of the Saturnian rings. By the way, the number density distributions of charged dust grains with different Q/m could also be acquired via numerical simulations. In this research, I used the Runge-Kutta 4th order method and which with some concepts from the Monte Carlo method to calculate the trajectories and number densities of the charged dust grains, respectively. The charge was fixed for all the orbital motion. However, I also tested the trajectories and number densities of charged dust grains affected by the shadow effect, and the charge properties of charged dust grains would be different instead of fixed. According to the results, when Q/m≥10^-4 e/mP, charged dust grains would precipitate into the upper atmosphere of Saturn via siphon flow if the injected positions of which were smaller than the stability critical radius (rc=1.53 RS). Besides, perhaps the ionosphere depletion of Saturnian equator was due to the injection of charged dust grains which with Q/m between 10^-6–10^-7 e/mP, and this phenomenon was observed via the Cassini radio occultation measurements. Furthermore, if charged dust grains did the orbital motion with the shadow effect, then something was different from purely positively or negatively charged dust grains did. The trajectories of charged dust grains within the Encke Gap could provide the information about the orbital stability via the relation between Q/m and angular velocity. However, there has not been in-situ observation near the ring plane until now, so this research work not only provides the cornerstone for the future observational model but also interprets some phenomena which happened to the upper atmosphere of Saturn, Saturnian ring system, and the interaction between Saturnian ring system and Saturn.en_US
DC.subject土星zh_TW
DC.subject土星環zh_TW
DC.subject磁場zh_TW
DC.subject帶電塵埃粒子zh_TW
DC.subject倫吉-庫塔法zh_TW
DC.subject蒙地卡羅法zh_TW
DC.subjectSaturnen_US
DC.subjectSaturnian ringsen_US
DC.subjectmagnetic fielden_US
DC.subjectcharged dust grainsen_US
DC.subjectRunge-Kutta methoden_US
DC.subjectMonte Carlo methoden_US
DC.title土星環鄰近地區之帶電塵埃粒子動力學zh_TW
dc.language.isozh-TWzh-TW
DC.titleDynamics of Charged Dust Grains in the Vicinity of the Saturnian Ringsen_US
DC.type博碩士論文zh_TW
DC.typethesisen_US
DC.publisherNational Central Universityen_US

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