对火星轨道变化问题的最后解释(6/24)

  【死在火星上】小说免费阅读,请收藏 全本免费小说【qbmfxs.com】

  (本部分涉及比较复杂的积分计算,作者君就不贴上来了,贴上来了起点也不一定能成功显示。)

  Numerical method

  We utilize a second-order Wisdom–Holman symplectic map as our main integration method (Wisdom & Holman 1991; Kinoshita, Yoshida & Nakai 1991) with a special start-up procedure to reduce the truncation error of angle variables,‘warm start’(Saha & Tremaine 1992, 1994).

  The stepsize for the numerical integrations is 8 d throughout all integrations of the nine planets (N±1,2,3), which is about 1/11 of the orbital period of the innermost planet (Mercury). As for the determination of stepsize, we partly follow the previous numerical integration of all nine planets in Sussman & Wisdom (1988, d) and Saha & Tremaine (1994, 225/32 d). We rounded the decimal part of the their stepsizes to 8 to make the stepsize a multiple of 2 in order to reduce the accumulation of round-off error in the computation processes. In relation to this, Wisdom & Holman (1991) performed numerical integrations of the outer five planetary orbits using the symplectic map with a stepsize of 400 d, 1/ of the orbital period of Jupiter. Their result seems to be accurate enough, which partly justifies our method of determining the stepsize. However, since the eccentricity of Jupiter (∼) is much smaller than that of Mercury (∼), we need some care when we compare these integrations simply in terms of stepsizes.

 

本章未完,点击[下一页]继续阅读-->>

温馨提示
  书友您好!程序猿书吧[cxysb.com] 是本站的备用域名及备用网站,用于公布本站的最新可用域名。如果您使用的域名无法访问,那么点击 程序猿书吧[cxysb.com] 域名可以帮您回到本站。如遇到内容无法显示或者显示不全,乱码错字,请退出阅读模式或畅读模式即可正常阅读。