Resonant Orbits Characteristics of Solar Sails Near the L2 Point in the Earth–Moon System

Aeronautical and Space-Rocket Engineering


Аuthors

Yu W. *, Starinova O. L.**

Samara National Research University named after Academician S.P. Korolev, 34, Moskovskoye shosse, Samara, 443086, Russia

*e-mail: yussau@foxmail.com
**e-mail: solleo@mail.ru

Abstract

As part of future lunar exploration and development projects, relay satellites for communication between the Earth and the Moon, especially the far side and polar regions of the Moon, where permanent bases are planned to be built, are attracting significant interest. This work is devoted to studying the characteristics of resonant orbits of solar sails near the L2 point in the Earth-Moon system, which are considered as potential trajectories for Earth-Moon relay satellites. A method is formulated in this article to ascertain resonant orbits near the L2 point, employing the multiple shooting method to solve a two-point boundary value problem with the goal of closing the spacecraft's trajectory to form a periodic orbit. Those resonant orbits formed based on Lyapunov orbits as initial approximations in two-point boundary value problems are called Lyapunov conformal orbits, and orbits formed based on halo orbits are called halo conformal orbits. An exploration is also executed on how resonant orbits vary concerning solar sail control variables, encompassing the initial position of the Sun, the magnitude of the nominal acceleration from light pressure and the installation angles of the solar sails. In result, such conclusions were obtained: 1. the influence of the initial position of the Sun divides the resonant orbits into different groups with different configurations; 2. the influence of the magnitude of the nominal acceleration determines the displacement of resonant orbits relative to natural periodic orbits, and Lyapunov conformal orbits have different changing trends of displacement compared with halo conformal orbits; 3. the influence of the installation angles of the solar sails mainly determines the displacement of the resonant orbits relative to natural periodic orbits in the out-of-plane direction, and for all orbits the maximum displacements obtain extreme values at ±35,26°.
 As a result of the research, the types and number of periodic orbits for placing Earth-Moon relay satellites were expanded, and dependencies for changes in resonant orbits were obtained. It should be noted that, in contrast to the orbits of traditional spacecrafts, the positions of spacecrafts with solar sails in resonant orbits are time dependent. Therefore, orbital phasing turns out to be an important component in the mission of insertion into a resonant orbit and requires additional research.

Keywords:

resonant orbit, solar sail, L2 libration point, Earth-Moon system, multiple shooting method, initial position of the Sun, nominal acceleration magnitude, solar sail installation angles

References

  1. Heidmann J. A proposal for a radio frequency interference-free dedicated lunar far side crater for high sensitivity radioastronomy: programmatic issues. Acta Astronautica, 2000, vol. 46, no. 8, pp. 555–558. DOI: 10.1016/S0094-5765(00)00002-3
  2. Li S., Lucey P.G., Milliken R.E. et al. Direct evidence of surface exposed water ice in the lunar polar regions. Proceedings of the National Academy of Sciences, 2018, vol. 115, no. 36, pp. 8907–8912. DOI: 10.1073/pnas.1802345115
  3. Breakwell J.V., Brown J.V. The ‘Halo’ family of 3-dimensional periodic orbits in the Earth-Moon restricted 3-body problem. Celestial Mechanics, 1979, vol. 20, no. 4, pp. 389-404. DOI: 10.1007/BF01230405
  4. Grebow D. Generating periodic orbits in the circular restricted three-body problem with applications to lunar south pole coverage, MSAA Thesis, West Lafayette, School of Aeronautics and Astronautics, Purdue University, 2006, 165 p.
  5. Kim M., Hall C.D. Lyapunov and halo orbits about L2. AAS/AIAA Astrodynamics Specialist Conference (30 July – 02 August 2001; Quebec City, Canada), vol. 109, pp. 349-366.
  6. Richardson D.L. Halo orbit formulation for the ISEE-3 mission. Journal of Guidance, Control, and Dynamics, 1980, vol. 3, no. 6, pp. 543-548. DOI: 10.2514/3.56033
  7. Serban R., Koon W.S., Lo M.W. et al. Halo orbit mission correction maneuvers using optimal control. Automatica, 2002, vol. 38, no. 4, pp. 571-583. DOI: 10.1016/S0005-1098(01)00279-5
  8. Gao S., Zhou W.Y., Zhang L. et al. Trajectory design and flight results for Chang’e 4-relay satellite. Scientia Sinica Technologica, 2019, vol. 49, no. 2, pp. 156–165. DOI: 10.1360/N092018-00393
  9. Jianfeng D., Xie L.I., Cuilan L.I., Zhaokui W. Orbit determination and analysis of Chang'E-4 relay satellite on mission orbit. Journal of Deep Space Exploration, 2019, vol. 6, no. 3, pp. 247–253.
  10. Lihua Z., Liang X., Ji S. One Year On-orbit Operation of Queqiao Lunar Relay Communications Satellite. Aerospace China, 2019, vol. 3.
  11. Polyakhova E.N. Kosmicheskii polet s solnechnym parusom (Space flight with a solar sail). 2nd ed. Moscow, URSS, 2010, 302 p.
  12. Garwin R.L. Solar Sailing: A Practical Method of Propulsion within the Solar System. Jet Propulsion, 1958, vol. 28, no. 3, pp. 188-190.
  13. Kirpichnikov S.N., Kirpichnikova E.S., Polyakhova E.N., Shmyrov A.S. Planar heliocentric roto-translatory motion of a spacecraft with a solar sail of complex shape. Celestial Mechanics and Dynamical Astronomy, 1995, no. 63, pp. 255-269.
  14. Spieth D., Zubrin R. Ultra-Thin Solar Sails for Interstellar Travel. Phase I Final Report. NASA Institute for Advanced Concepts, 1999, 32 p.
  15. Tsuda Y., Mori O., Funase R. et al. Achievement of IKAROS—Japanese deep space solar sail demonstration mission. Acta Astronautica, 2013, vol. 82, no. 2, pp. 183–188. DOI: 10.1016/j.actaastro.2012.03.032
  16. Spencer D.A., Betts B., Bellardo J.M. et al. The LightSail 2 solar sailing technology demonstration. Advances in Space Research, 2020, vol. 67, no. 9, pp. 2878-2889. DOI: 10.1016/j.asr.2020.06.029
  17. Gong S., Li J. Solar sail heliocentric elliptic displaced orbits. Journal of Guidance, Control, and Dynamics, 2014, vol. 37, no. 6, pp. 2021-2026. DOI: 10.2514/1.G000660
  18. Bookless J., McInnes C. Control of Lagrange point orbits using solar sail propulsion. Acta Astronautica, 2008, vol. 62, no. 2-3, pp. 159-176.
  19. Heiligers J., Hiddink S., Noomen R., McInnes C.R. Solar sail Lyapunov and Halo orbits in the Earth–Moon three-body problem. Acta Astronautica, 2015, vol. 116, pp. 25-35. DOI: 10.1016/j.actaastro.2015.05.034
  20. Richardson D.L. A note on a Lagrangian formulation for motion about the collinear points. Celestial Mechanics, 1980, vol. 22, no. 3, pp. 231-236. DOI: 10.1007/BF01229509
  21. Howell K.C. Families of orbits in the vicinity of the collinear libration points. AIAA/AAS Astrodynamics Specialist Conference and Exhibit (10-12 August 1998; Boston, MA, USA). DOI: 10.2514/6.1998-4465
  22. Bock H.G., Plitt K.J. A multiple shooting algorithm for direct solution of optimal control problems. IFAC Proceedings Volumes, 1984, vol. 17, no. 2, pp. 1603-1608. DOI: 10.1016/S1474-6670(17)61205-9
  23. Gómez G., Masdemont J.J., Mondelo J.M. Libration point orbits: a survey from the dynamical point of view. Libration point orbits and applications, 2003, pp. 311-372. DOI: 10.1142/9789812704849_0016

mai.ru — informational site of MAI

Copyright © 1994-2024 by MAI