双小行星系统中主天体的自旋轨道耦合

Hanlun Lei
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摘要

自旋轨道耦合在双小行星系统中非常普遍,对椭球二次的情况也进行了广泛的研究。由于角动量的交换,当轨道角动量和旋转角动量的量级比较接近时,动力学耦合会更强。因此,自旋轨道耦合效应在椭球二次粒子和主粒子上有很大不同。本研究建立了一个以偏心率为基础的高阶哈密顿模型,以研究双小行星系统中椭圆形主星的自旋轨道耦合效应。研究结果表明,椭球主星的自旋轨道耦合问题存在两种自旋平衡,而椭球副星只有一种。特别是通过经典钟摆近似和绝热近似(Wisdom 的微扰处理)进一步研究了 1:1 和 2:3 自旋轨道共振。结果表明,总角动量存在一个临界值,在该值附近,钟摆近似无法起作用。当总角动量处于临界值的两侧时,动力学结构完全不同。
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Spin–orbit coupling of the primary body in a binary asteroid system

Spin–orbit coupling is widespread in binary asteroid systems, and it has been widely studied for the case of ellipsoidal secondary. Due to angular momentum exchange, dynamical coupling is stronger when the orbital and rotational angular momenta are closer in magnitudes. Thus, the spin–orbit coupling effects are significantly different for ellipsoidal secondaries and primaries. In the present work, a high-order Hamiltonian model in terms of eccentricity is formulated to study the effects of spin–orbit coupling for the case of ellipsoidal primary body in a binary asteroid system. Our results show that the spin–orbit coupling problem for the ellipsoidal primary holds two kinds of spin equilibrium, while there is only one for the ellipsoidal secondary. In particular, 1:1 and 2:3 spin–orbit resonances are further studied by taking both the classical pendulum approximation and adiabatic approximation (Wisdom’s perturbative treatment). It shows that there is a critical value of total angular momentum, around which the pendulum approximation fails to work. Dynamical structures are totally different when the total angular momentum is on two sides of the critical value.

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