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Analytical Solutions for Planet-scattering Small Bodies

  • Authors: Yukun Huang, 宇坤 黄, Brett Gladman, Eiichiro Kokubo, 英一郎 小久保

Yukun Huang et al 2026 The Astronomical Journal 171 .

  • Provider: AAS Journals

Caption: Figure 1.

Schematic illustration of the 3D scattering geometry in a planet-centered corotating frame. The z-axis (﹩\hat{{\boldsymbol{k}}}﹩) points out of the orbital plane, while the x-axis (﹩\hat{{\boldsymbol{i}}}﹩) and y-axis (﹩\hat{{\boldsymbol{j}}}﹩) are aligned respectively with the instantaneous radial and transverse directions of the planet at the time of encounter. In this coordinate system, rp lies entirely along the x-axis, and vp (the planet’s velocity, solid black arrow) lies along the y-axis. The small-body’s heliocentric velocity vector at the intersection vcross (solid red arrow) is the vector sum of the relative-velocity vector v (solid blue arrow) and vp. The vector U = v/vp is the normalized relative velocity. The two angles θ (the polar angle from vp) and ϕ (the azimuth angle of v in the xz plane) fully specify the direction of the relative-velocity vector.

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