Beispiel #1
0
def evolve_system(particles):
    """
    Evolves the system using the Hermite integrator.


    Parameters
    ----------
    particles: amuse.datamodel.particles.Particles instance

    """
    times = numpy.linspace(0.0001, args.time, args.steps) | u.yr

    intr = Hermite(nbody_to_si(particles.total_mass(), 1 | u.AU))
    intr.particles.add_particles(particles)

    energy_begin = intr.get_total_energy()

    if args.dt is not None:
        intr.set_dt_param(args.dt)

    for t in times:
        intr.evolve_model(t)
        energy_error = (intr.get_total_energy() - energy_begin) / energy_begin
        print(intr.get_time_step().in_(u.day), intr.get_time().in_(u.yr))
        print(energy_error)

    print("energy error:{}".format(energy_error))

    intr.stop()
def evolve_system(particles):
    """
    Evolves the system using the Hermite integrator.


    Parameters
    ----------
    particles: amuse.datamodel.particles.Particles instance

    """
    times = numpy.linspace(0.0001, args.time, args.steps) |u.yr

    intr = Hermite(nbody_to_si(particles.total_mass(), 1 | u.AU))
    intr.particles.add_particles(particles)

    energy_begin = intr.get_total_energy()

    if args.dt is not None:
        intr.set_dt_param(args.dt)

    for t in times:
        intr.evolve_model(t)
        energy_error = (intr.get_total_energy() - energy_begin)/energy_begin
        print(intr.get_time_step().in_(u.day), intr.get_time().in_(u.yr))
        print(energy_error)
      

    print("energy error:{}".format(energy_error))

    intr.stop()