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HITEN - Computational Toolkit for the Circular Restricted Three-Body Problem

Project description

HITEN

HITEN - Computational Toolkit for the Circular Restricted Three-Body Problem

PyPI version

Overview

HITEN is a research-oriented Python library that provides an extensible implementation of high-order analytical and numerical techniques for the circular restricted three-body problem (CR3BP).

Examples

  1. Parameterisation of periodic orbits and their invariant manifolds

    The toolkit constructs periodic solutions such as halo orbits and computes their stable and unstable manifolds.

    from hiten import System
    
    system = System.from_bodies("earth", "moon")
    l1 = system.get_libration_point(1)
    
    orbit = l1.create_orbit("halo", amplitude_z=0.2, zenith="southern")
    orbit.correct(max_attempts=25)
    orbit.propagate(steps=1000)
    
    manifold = orbit.manifold(stable=True, direction="positive")
    manifold.compute()
    manifold.plot()
    

    Halo orbit stable manifold

    Figure 1 - Stable manifold of an Earth-Moon (L_1) halo orbit.

    Knowing the dynamics of the center manifold, initial conditions for vertical orbits can be computed and associated manifolds created. These reveal natural transport channels that can be exploited for low-energy mission design.

    from hiten import System, VerticalOrbit
    
    system = System.from_bodies("earth", "moon")
    l1 = system.get_libration_point(1)
    
    cm = l1.get_center_manifold(max_degree=10)
    cm.compute()
    
    initial_state = cm.ic(poincare_point=[0.0, 0.0], energy=0.6, section_coord="q3")
    
    orbit = VerticalOrbit(l1, initial_state=initial_state)
    orbit.correct(max_attempts=100)
    orbit.propagate(steps=1000)
    
    manifold = orbit.manifold(stable=True, direction="positive")
    manifold.compute()
    manifold.plot()
    

    Vertical orbit stable manifold

    Figure 2 - Stable manifold of an Earth-Moon (L_1) vertical orbit.

  2. Generating families of periodic orbits

    The toolkit can generate families of periodic orbits by continuation.

    from hiten import System
    from hiten.algorithms import StateParameter
    
     system = System.from_bodies("earth", "moon")
     l1 = system.get_libration_point(1)
    
     seed = l1.create_orbit('lyapunov', amplitude_x= 1e-3)
     seed.correct(max_attempts=25)
    
     target_amp = 1e-2 # grow A_x from 0.001 to 0.01 (relative amplitude)
     current_amp = seed.amplitude
     num_orbits = 10
    
     # Step in amplitude space (predictor still tweaks X component)
     step = (target_amp - current_amp) / (num_orbits - 1)
    
     engine = StateParameter(
         initial_orbit=seed,
         state=(S.X),     # underlying coordinate that gets nudged
         amplitude=True,  # but the continuation parameter is A_x
         target=(current_amp, target_amp),
         step=step,
         corrector_kwargs=dict(max_attempts=50, tol=1e-13),
         max_orbits=num_orbits,
     )
     engine.run()
    
     family = OrbitFamily.from_engine(engine)
     family.propagate()
     family.plot()
    

    Lyapunov orbit family

    Figure 3 - Family of Earth-Moon (L_1) Lyapunov orbits.

  3. Generating Poincaré maps

    The toolkit can generate Poincaré maps for the centre manifold over various sections.

    from hiten import System
    
    system = System.from_bodies("earth", "moon")
    l1 = system.get_libration_point(1)
    
    cm = l1.get_center_manifold(max_degree=12)
    cm.compute()
    
    pm = cm.poincare_map(energy=0.7, section_coord="q2", n_seeds=50, n_iter=100, seed_strategy="axis_aligned")
    pm.compute()
    pm.plot()
    

    Poincaré map

    Figure 4 - Poincaré map of the centre manifold of the Earth-Moon (L_1) libration point using the (q_2=0) section.

  4. Generating invariant tori

    Hiten can generate invariant tori for periodic orbits.

    from hiten import System
    from hiten.algorithms import InvariantTori
    
     system = System.from_bodies("earth", "moon")
     l1 = system.get_libration_point(1)
    
     orbit = l1.create_orbit('halo', amplitude_z=0.3, zenith='southern')
     orbit.correct(max_attempts=25)
     orbit.propagate(steps=1000)
    
     torus = InvariantTori(orbit)
     torus.compute(scheme='linear', epsilon=1e-2, n_theta1=256, n_theta2=256)
     torus.plot()
    

    Invariant tori

    Figure 5 - Invariant torus of an Earth-Moon (L_1) quasi-halo orbit.

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