A time and fuel pulse optimal traversal method for the local range of space objects observed by spacecraft on-orbit service
A space-based, local-scale technology, applied in instrumentation, 3D position/course control, adaptive control, etc., to solve problems such as increased mission execution time, spacecraft mass and volume constraints, etc.
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specific Embodiment approach 1
[0032] Specific implementation mode 1: The time and fuel pulse optimal traversal method of a spacecraft on-orbit service observation space target local range according to this implementation mode is specifically prepared according to the following steps:
[0033] Step 1. Without considering perturbation, when the target s is in a circular orbit, the relative orbital motion model of the tracking spacecraft is obtained and described as the C-W equation; according to the C-W equation, the relative position r(t) and relative velocity of the tracking spacecraft are obtained The state transition equation of ;
[0034] Step 2. Determine the direction of the center of the local range to be observed as the direction of the observation center line according to the task requirements. In two mutually perpendicular directions in a plane perpendicular to the observation center line, there is an angle range of M°, and the M° angle The range of angles is equally divided into l×l subdivided g...
specific Embodiment approach 2
[0046] Specific embodiment two: the difference between this embodiment and specific embodiment one is: in step one, when the perturbation is not considered, when the target s is in a circular orbit, the relative orbital motion model of the tracking spacecraft is described as a C-W equation; According to the C-W equation, the relative position r(t) and relative velocity of the tracking spacecraft are obtained The specific process of the state transition equation is:
[0047] Let the target be s, and the tracking spacecraft be c; let the spacecraft serve the observation space target in orbit, that is, the target s is in a near-circular orbit, and take the orbital coordinate system s-xyz of the target as the relative motion coordinate system; the relative motion coordinate system The origin is fixed to the center of mass of the target and moves along the orbit with the center of mass of the target, the x-axis of the relative motion coordinate system and the geocentric vector r o...
specific Embodiment approach 3
[0068] Embodiment 3: The difference between this embodiment and Embodiment 1 or 2 is that the traversal order of the spiral form in Step 3 is specifically:
[0069] When l is an even number, the starting grid selects any one of the four vertex grids in all the subdivided grids, and performs the traversal of the spiral form in the clockwise or counterclockwise direction;
[0070] If any one of the four grids in the middle of all the subdivision grids is selected, the helical traversal of the unscrewed form is performed in a clockwise or counterclockwise direction;
[0071] There are a total of 16 optional traversal sequences for spiral traversal in the form of precession and spiral traversal in the form of precession, and one of the 16 optional traversal sequences can be selected arbitrarily according to the actual situation;
[0072] Taking the subdivision grid when l is an even number as an example, the starting grid can choose A, B, C, D, E, F, G, One of the eight grids of ...
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