Multiple-Revolution Solutions of the Transverse-Eccentricity-Based Lambert Problem
Multiple-Revolution Solutions of the Transverse-Eccentricity-Based Lambert Problem
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DOI:
10.2514/1.45041
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发表时间:
2010
影响因子:
2.6
通讯作者:
Quan He;Jun Yu Li;Chao Han
中科院分区:
文献类型:
--
作者:
Quan He;Jun Yu Li;Chao Han
T HIS Engineering Note follows a previous paper in which Avanzini [1] presented a transverse-eccentricity-vector-based algorithm to solve the classical Lambert problem: that is, the determination of a transfer orbit having a specified flight time and connecting two position vectors [2]. In Avanzini’s [1] paper, the eccentricity vector of the transfer orbit can be decomposed into a constant component parallel to the chord connecting the two points and a variable transverse component in the direction perpendicular to it on the orbit plane. Given the two fixed position vectors, the transfer time can be expressed as a function of the transverse eccentricity eT. Compared with the elegant Battin’s method, the derivation of this simple Lambert algorithm seems to be considerably less demanding from the mathematical standpoint and physically more intuitive [1]. However, with the only consideration of direct-transfer arcs, neither the explicit expression of the derivative of the transfer time with respect to the transverse eccentricity nor the multiple-revolution solutions based on the novel method were given in [1]. The multiple-revolution Lambert’s problem has been being discussed since the 1980s [3]. After the 1990s, mainly based on Ochoa’s works [4], many experts studied the multiple-revolution using the classical Lagrange formulation for an elliptic transfer orbit, where the transfer time was expressed as a function of semimajor axis. Prussing [5] developed a minimum-fuel multiple-revolution algorithm for an elliptic orbit to determine all the possible transfer trajectories, based on the classical Lagrange formulation. Also based on this formulation, Shen andTsiotras [6] presented aminimumV, fixed-time, two-impulse transfer algorithm between two coplanar circular orbits. In Shen and Tsiotras’s algorithm, only two of the multiple-revolution solutions need to be calculated and compared to obtain the minimum-cost transfer orbit. In addition to the Lagrange formulation method, it is also possible to use universal variables to solve the multiple-revolution problem [7]. Han and Xie [8] also presented a homologous algorithm to obtain the multiple-revolution solutions using these variables. In [8], the transfer timewaswritten as a function of universal variable z, for which the value is limited to the boundary 4N 2 < z < 4 N 1 2 2