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    • Home (overview)
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  • Cislunar glossary (terms & definitions)

    • Cislunar Space Glossary
    • Dynamics models

      • Circular Restricted Three-Body Problem (CR3BP)
      • CR3BP with Low-Thrust (CR3BP-LT)
      • A2PPO (Attention-Augmented Proximal Policy Optimization)
      • Curriculum Learning
      • Low-Thrust Transfer MDP Formulation
      • Generalized Advantage Estimation (GAE)
      • Direct Collocation
      • Birkhoff-Gustavson Normal Form
      • Central Manifold
      • Action-Angle Variables
      • Poincaré Section
      • Clohessy-Wiltshire (CW) Equation
      • Patched Method (拼接法)
      • Continuation (延拓)
      • Differential Correction (微分修正)
      • Poincaré Map (庞加莱图)
      • Impulsive Maneuver (脉冲机动)
      • Zero-Velocity Surface
      • Hill Three-Body Problem
      • Bicircular Four-Body Problem
      • Quasi-Bicircular Four-Body Problem
      • Strobe Map
      • Stability Set
      • Backward Stability Set
      • Capture Set
      • /en/glossary/dynamics/batch-deployment.html
      • /en/glossary/dynamics/state-dependent-tsp.html
      • /en/glossary/dynamics/q-law.html
      • /en/glossary/dynamics/mass-discontinuity.html
      • /en/glossary/dynamics/equinoctial-elements.html
      • /en/glossary/dynamics/dynamic-programming.html
      • /en/glossary/dynamics/coasting-arc.html
    • Mission orbits

      • Distant Retrograde Orbit (DRO)
      • Near-Rectilinear Halo Orbit (NRHO)
      • Earth-Moon L1/L2 Halo Orbit (EML1/EML2 Halo)
      • DRO Constellation
      • Orbit Identification
      • Transfer Orbit (转移轨道)
      • Perilune (近月点)
      • Apolune (远月点)
      • Retrograde (逆行)
      • Prograde (顺行)
      • Parking Orbit (停泊轨道)
      • Free-Return Trajectory (自由返回轨道)
      • Halo Orbit (Halo 轨道)
      • Lissajous Orbit (Lissajous 轨道)
      • Lyapunov Orbit (Lyapunov 轨道)
      • Cycler Trajectory
      • Multi-Revolution Halo Orbit
      • Ballistic Capture Orbit
      • Low-Energy Transfer Orbit
      • Full Lunar Surface Coverage Orbit
      • /en/glossary/orbits/hub-and-spoke.html
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      • Weak Stability Boundary / WSB (弱稳定边界)
      • /en/glossary/other/libration-point.html
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      • /en/glossary/other/orbital-residence-platform.html
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Halo Orbit

Author: CislunarSpace

Website: https://cislunarspace.cn

Definition

A Halo orbit is a three-dimensional periodic orbit surrounding a libration point, appearing as a halo or ring shape in the synodic reference frame. Halo orbits are a class of exact periodic solutions in the Circular Restricted Three-Body Problem (CR3BP), existing primarily near the L1, L2, and L3 libration points of the Earth-Moon system. Among these, Halo orbits near the Earth-Moon L2 point have the most extensive applications in current deep-space exploration.

Key Elements

Dynamic Characteristics of Halo Orbits

Halo orbits have the following characteristics in the CR3BP framework:

  • Three-dimensional motion: Unlike planar Lyapunov orbits, Halo orbits have large-amplitude oscillations in the xOyxOyxOy plane combined with significant periodic motion in the zzz direction, forming ring-shaped trajectories in three-dimensional space
  • Periodicity: Halo orbits are strictly periodic, precisely closing in the synodic reference frame
  • Symmetry: Standard Halo orbits are symmetric about the xOzxOzxOz plane; when the orbit crosses this plane, the xxx and zzz velocity components are zero
  • Amplitude parameterization: Halo orbit families are described by the amplitude parameter AzA_zAz​ (maximum displacement in the zzz direction); larger amplitude means the orbit is farther from the libration point

The relationship between Halo orbit period TTT and amplitude can be approximately expressed as:

T≈T0+αAz2T \approx T_0 + \alpha A_z^2 T≈T0​+αAz2​

where T0T_0T0​ is the natural period of linearized motion near the libration point and α\alphaα is a coefficient related to system parameters.

Linear Approximation of Halo Orbits

Near the libration point, the CR3BP equations of motion can be linearized. For collinear libration points (L1, L2, L3), the linearized motion has two real eigenvalues in the plane (corresponding to stable/unstable manifolds) and a pair of conjugate imaginary eigenvalues (corresponding to periodic oscillation), with another pair of conjugate imaginary eigenvalues in the zzz direction. The existence condition for Halo orbits is that the oscillation frequencies in-plane and in the zzz direction satisfy a resonance relationship:

ωz/ωxy≈1\omega_z / \omega_{xy} \approx 1 ωz​/ωxy​≈1

Richardson (1980) used the Lindstedt-Poincaré method to derive a third-order approximate analytical solution for Halo orbits, providing excellent initial guesses for numerically precise solutions.

Stability and Station-Keeping Control

Most Halo orbits are unstable -- their stable and unstable manifolds point toward and away from the orbit respectively. Therefore:

  • Spacecraft on Halo orbits require periodic station-keeping maneuvers
  • Control strategies are typically based on Floquet theory, eliminating components that grow along the unstable manifold
  • Typical station-keeping for L2 Halo orbits requires approximately several m/s per year

Near-Rectilinear Halo Orbit (NRHO)

NRHO is a special subclass of Halo orbits with extremely elongated shapes, where the perilune is close to the lunar surface and the apolune extends into deep space. NRHO is the target orbit for NASA's Gateway space station, combining the three-dimensional coverage advantages of Halo orbits with the communication/observation advantages of low perilune.

Application Value

Halo orbits have core application value in cislunar missions:

  • Gateway space station: NASA's Artemis program Gateway station is deployed in a lunar L2 NRHO
  • Relay communications: L2 Halo orbits can provide continuous communication relay for the lunar far side
  • Scientific observation: Halo orbits offer unique observation geometries, suitable for space science and astronomical observation
  • Deep space exploration stepping stone: Halo orbits can serve as transfer orbits for deeper space missions

Related Concepts

  • Earth-Moon L1/L2 Halo Orbit (EML1/EML2 Halo)
  • Near-Rectilinear Halo Orbit (NRHO)
  • Lissajous Orbit
  • Lyapunov Orbit
  • Circular Restricted Three-Body Problem (CR3BP)

References

  • Richardson D L. Analytic construction of periodic orbits about the collinear points[J]. Celestial Mechanics, 1980, 22(3): 241-253.
  • Farquhar R W. The utilization of halo orbits in advanced lunar operations[R]. NASA, 1971.
  • Qiao C, Long X, Yang L, et al. Orbital parameter characterization and objects cataloging for Earth-Moon collinear libration points[J]. Chinese Journal of Aeronautics, 2025.
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Last Updated: 4/29/26, 11:30 AM
Contributors: Cron Job
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