首页> 外文会议>AAS/AIAA Astrodynamics Conference; 20050807-11; South Lake Tahoe,CA(US) >PERIODIC ORBITS IN THE VICINITY OF THE EQUILATERAL POINTS OF THE RESTRICTED FULL THREE-BODY PROBLEM
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PERIODIC ORBITS IN THE VICINITY OF THE EQUILATERAL POINTS OF THE RESTRICTED FULL THREE-BODY PROBLEM

机译:受限的三体问题等边点附近的周期轨道

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Periodic orbits are computed for a particle in the gravitational field of a binary system. First, the equations of motion are derived. One of the bodies is modeled as a sphere and the other as a constant density tri-axial ellipsoid. Previous work has investigated the dynamics and stability of relative equilibria of the binary system itself. The dynamics of a particle in the gravitational field of a binary system have also been studied. Equilibrium solutions near L_4, L_5 and their stability have been characterized. In the current model, the stability of these points are functions of the mass ratio, the distance between the bodies and the size parameters of the ellipsoid. In this paper, the binary system is in a non-synchronous motion where the ellipsoid spins about its maximum moment of inertia while being in mutual orbit about the sphere. In order to find periodic orbits, a Poincare map reduction method is used with the time periodic nonlinear equations of motion of the ellipsoid-sphere system. To provide more analytical insights on the behavior of this periodic system, a perturbation method is also applied. As an approximation, the gravity field of the ellipsoid body is expanded in terms of spherical harmonics. Numerical simulations show that stable periodic orbits exist for low values of the mass ratio. The ratio between the orbit period of the binary system and the rotation period of the primary is now an added free parameter of the system. We find it plays a strong role in determining the stability and size of the resulting periodic orbits. The stability region is reduced compared to known results of the Restricted Three-Body Problem and the synchronous case of the Restricted Full Three-Body Problem.
机译:计算二元系统引力场中粒子的周期性轨道。首先,导出运动方程。其中一个实体建模为球体,另一个实体建模为恒密度三轴椭圆体。先前的工作已经研究了二元系统本身的相对平衡的动力学和稳定性。还研究了二元系统引力场中粒子的动力学。表征了L_4,L_5附近的平衡解及其稳定性。在当前模型中,这些点的稳定性取决于质量比,物体之间的距离以及椭球的尺寸参数。在本文中,二元系统处于非同步运动中,椭球在绕球体相互轨道的同时绕其最大惯性矩旋转。为了找到周期轨道,将庞加莱映射约简方法与椭球体系统的时间周期非线性运动方程一起使用。为了提供有关此周期系统行为的更多分析见解,还应用了一种摄动方法。近似地,椭球体的重力场根据球谐函数扩展。数值模拟表明,低质量比值存在稳定的周期轨道。现在,双星系统的轨道周期与原边旋转周期之间的比率是系统的附加自由参数。我们发现它在确定所产生的周期性轨道的稳定性和大小方面发挥着重要作用。与限制三体问题的已知结果和限制全三体问题的同步情况相比,减小了稳定区域。

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