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논문 기본 정보

자료유형
학위논문
저자정보

이상철 (충남대학교, 忠南大學校 大學院)

지도교수
석진영
발행연도
2014
저작권
충남대학교 논문은 저작권에 의해 보호받습니다.

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이 논문의 연구 히스토리 (4)

초록· 키워드

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The Soviet Union''s Lunar 1 was the first human-made object to reach on the Moon on 13 September 1959. The first manned mission to land on the Moon on 20 July 1969. Since six manned U.S. landing, no soft landing had been happened from 1976 until 14 December 2013. Chang''e 3 was launched on 2 December 2013 aboard a Long March 3B rocket, and successfully landed on the Moon on 14 December 2013. The lunar rover named Yutu is first rover to operate there since the Soviet Lunokhod 2 ceased operation on 11 May 1973. Joseph Louis Lagrange published an "Essay on the three-body problem". In this essay, he demonstrated two special constant-pattern solutions, the collinear and the equilateral for any three masses with circular orbits. Indeed, the german astronomer Max Wolf discovered Achilles of the trojan asteroids in the L4 Lagrange point of the Sun-Jupiter system.
Orbits around Lagrange points offer advantages for performing certain spacecraft missions. For example the Sun-Earth L1 point is useful for observations of the Sun as the Sun is always visible without obstructions by the Earth or the Moon. The Sun-Earth L2 point is useful for astronomy missions using space telescope with no sun light interference. In 1968, Farquhar first suggested a spacecraft in a halo orbit on the far side of the Moon near the Earth-Moon L2 point as a communication relay station for an Apollo mission to the far side of the Moon. The Earth-Moon L2 point also used a gateway to explorer the solar system. Also Earth-Moon L2 halo orbit can be used for as an orbit of lunar space station to supply for a space explorer. And it might be needed to land on the Moon for gathering lunar resources. For this reason, a transfer strategy from earth and halo orbit and a transfer strategy halo orbit to lunar surface should be determined with taking into account fuel saving.
In this paper, in order to get the maneuver planning for the lunar soft landing via the Earth-Moon L2 halo orbit, the mission the surface of the Moon is consist of two scenario. The first scenario is orbit transfers from GTO(Geostationary Transfer Orbit) to the Earth-Moon L2 Halo orbit, performing three maneuvers in the GTO in order to make a transfer to GEO, then performing a maneuver in the GEO to leave to the Earth-Moon L2 Halo orbit, then performing an additional maneuver to become injected on Halo orbit. The lowest total burn for this type of direct transfer is a Hohmann transfer from the GEO to the Halo orbit. The second scenario is orbit transfers from the Earth-Moon L2 Halo orbit to lunar soft landing, performing Halo deorbit maneuver, the lunar orbit injection maneuver, lunar low circular orbit maneuver, powered descent maneuver, braking maneuver and soft landing maneuver. In this paper, the reference trajectory was calculated using differential corrector, and the global optimization was used in order to get orbit maneuver parameters such as maneuver time, magnitude and direction.
A spacecraft may face a collision with space debris or astroid, which result in catastrophic mission failure or a loss of human life. A global optimization algorithm such as genetic algorithm, simulated annealing, and pattern search is used to obtain the maneuver magnitude, direction and time to reach a target orbit, and to reduce the probability of collision with uncontrolled objects.
As a result, in non-linear problem, the differential corrector can lead us to the wrong answer and diverge because of initial guess values. Also sequential quadratic programming based on the derivative may go into local minimum solution. It is found that the utilization of global optimization has benefit to obtain solution for orbit maneuver in near earth orbit mission and beyond the earth orbit with constrained problem because of derivative free. But it have a disadvantage in expensive computational time.

목차

1 서론1
1.1 연구 동기1
1.2 선행 연구6
1.3 연구 내용9
1.4 논문 구성10
2 운동방정식11
2.1 좌표계 설정11
2.2 케플러 궤도요소13
2.3 2체 문제14
2.4 3체와 n체문제15
2.5 원형제한3체문제(Circular Restricted Three Body Problem)17
2.6 달의 특성28
3 궤도기동31
3.1 동일평면에서의 접선분사를 이용한 궤도기동31
3.2 동일평면에서의 비접선분사를 이용한 궤도기동33
3.3 궤도면 변경기동33
3.4 복합궤도기동35
3.5 Patched Conic Approximation35
3.6 지구-달 할로궤도 전이40
3.7 GTO를 사용한 정지궤도 전이42
3.8 달착륙43
3.9 외부교란력45
4 기동계획 탐색법49
4.1 차분보정49
4.2 SQP52
4.3 유전 알고리즘53
4.4 모의 담금질54
4.5 패턴서치 알고리즘56
5 시뮬레이션58
5.1 GEO를 경유한 할로궤도 기동계획59
5.2 할로궤도에서의 달연착륙 기동 계획85
5.3 GEO 경도획득궤도에서의 충돌회피108
5.4 충돌회피를 고려한 할로궤도 투입기동 계획117
6 결론128
참고 문헌130

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