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OPTIMAL IMPULSIVE ORBITAL MANEUVER BETWEEN NONCOPLANAR NONCOAXIAL ORBITS WITH OR WITHOUT TIME CONSTRAINT

机译:具有时间约束或没有时间约束的非共面非共轴轨道之间的最优脉冲轨道操纵

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In order to solve the problem of optimal impulsive orbital 3D maneuver with or without time constraint one must first solve theoptimal condition's equations. There are different and numerous modes of geometry, all of these modes must be considered.Solving this problem with the geometric modes has, to my knowledge, not been done before. In this paper the problem has beensolved in two states: with time constraint and no time constraint while considering all possible geometric modes. The purpose ofthis paper is solving the problem and achieving the global solution. For considering all possible modes of geometry, the relations ofoblique spherical triangle must be used. All necessary angles can be determined by using these relations. In this paper, 16 modes forexposure of initial orbit to final orbit and 16 modes for exposure of transfer orbit to initial and final orbits are classified. Then, theoptimal condition equations have been solved. Solving the equations led to only one local minimum and the global solution cannotbe identified. Therefore, the process is required to determine global solution. In this paper, the explicit equations have beenextracted which by using them, intermediary variables evaluated with respect to independent variables. Then, the function ofimpulse can be minimized to independent variables separately. The exact location of global solution can be determined byexamining the behavior of the function to the independent variables. Therefore, the global solution can be obtained. Finally, themethod is applied for the numerical example. The initial and final orbits is elliptical and non coplanar and elements of them arecertain. The example is solved in two modes of time constraint and no time constraint. In time constraint mode, the time of transfermust be 2500 seconds. In this mode some results have been verified by solving the Lambert problem. In the non time constraintmode, the total required impulse is less than the time constraint mode as expected. The solutions of two of these modes have beensimulated by MATLAB code. The results show acceptable accuracy and high-speed computing.
机译:为了解决有或没有时间限制的最佳脉冲轨道3D机动问题,必须首先解决 最佳条件方程。有多种不同的几何模式,必须考虑所有这些模式。 据我所知,用几何模式解决这个问题以前没有做过。本文的问题是 在两个状态下求解:在考虑所有可能的几何模式的情况下,有时间限制和无时间限制。的目的 本文正在解决问题并实现全球解决方案。在考虑所有可能的几何模式时, 必须使用倾斜的球形三角形。通过使用这些关系,可以确定所有必要的角度。本文介绍了16种模式 将初始轨道暴露于最终轨道和将转移轨道暴露于初始和最终轨道的16种模式进行了分类。然后, 最佳条件方程已解决。解方程只导致一个局部最小值,而整体解不能 被识别。因此,需要该过程来确定全局解决方案。在本文中,显式方程为 通过使用它们,提取相对于自变量的中间变量。然后, 可以将冲量分别最小化为自变量。全局解决方案的确切位置可以通过以下方式确定 检查函数对自变量的行为。因此,可以获得全局解决方案。最后, 方法应用于数值示例。初始轨道和最终轨道是椭圆形的和非共面的,并且它们的元素是 肯定。该示例以时间约束和无时间约束两种模式解决。在时间限制模式下,转移时间 必须是2500秒。在此模式下,通过解决Lambert问题已验证了一些结果。在无时间限制的情况下 模式,所需的总脉冲小于预期的时间限制模式。这两种模式的解决方案是 由MATLAB代码模拟。结果表明可接受的精度和高速计算。

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