コード例 #1
0
ファイル: star_to_sph.py プロジェクト: Ingwar/amuse
    def result(self):
        if self.pickle_file is None:
            self.retrieve_stellar_structure()
        else:
            self.unpickle_stellar_structure()

        if self.with_core_particle:
            self.setup_core_parameters()

        sph_particles = self.convert_to_SPH()
        if self.do_relax:
            for result_string in self.relax(sph_particles):
                print result_string

        specific_internal_energy, composition, mu = self.interpolate_internal_energy(
            sph_particles.position.lengths(),
            do_composition_too = self.do_store_composition
        )
        sph_particles.u = specific_internal_energy
        if self.do_store_composition:
            sph_particles.add_vector_attribute("composition", self.species_names)
            sph_particles.composition = composition
            sph_particles.mu = mu

        if self.with_core_particle and self.core_radius:
            core_particle = Particle()
            core_particle.mass = self.core_mass
            core_particle.position = [0.0, 0.0, 0.0] | units.m
            core_particle.velocity = [0.0, 0.0, 0.0] | units.m / units.s
            core_particle.radius = self.core_radius
            return StellarModelInSPH(gas_particles=sph_particles, core_particle=core_particle, core_radius=self.core_radius)
        return StellarModelInSPH(gas_particles=sph_particles, core_particle=None, core_radius=None)
コード例 #2
0
ファイル: XiTau.py プロジェクト: amusecode/amuse
def continue_evolution(sph_code, dynamics_code, t_end, n_steps, 
        relaxed_giant_output_base_name, do_energy_evolution_plot):
    print "Loading snapshots...",
    files = os.listdir("snapshots")
    files.sort()
    files = files[-4:]
    print files
    binary = read_set_from_file(os.path.join("snapshots", files[0]), format='amuse')
    gd_particles = read_set_from_file(os.path.join("snapshots", files[1]), format='amuse')
    sph_particles = read_set_from_file(os.path.join("snapshots", files[2]), format='amuse')
    
    snapshotfile = os.path.join("..", "giant_models", relaxed_giant_output_base_name + "_core.amuse")
    core_particle = read_set_from_file(snapshotfile, format='amuse')
    
    giant_model = StellarModelInSPH(
        gas_particles = sph_particles, 
        core_particle = gd_particles[0], 
        core_radius = core_particle.radius)
    
    view_on_giant = Particle()
    view_on_giant.position = [0]*3 | units.m
    view_on_giant.velocity = [0]*3 | units.m / units.s
    
    print "\nSetting up {0} to simulate inner binary system".format(dynamics_code.__name__)
    binary_system = prepare_binary_system(dynamics_code, binary)
    
    print "\nSetting up {0} to simulate giant in SPH".format(sph_code.__name__)
    giant_system = prepare_giant_system(sph_code, giant_model, view_on_giant, t_end, n_steps)
    
    print "\nEvolving with bridge between", sph_code.__name__, "and", dynamics_code.__name__
    evolve_coupled_system(binary_system, giant_system, t_end, n_steps, do_energy_evolution_plot, 
        previous_data = os.path.join("snapshots", files[3]))
    print "Done"
コード例 #3
0
ファイル: orbit_in_potential.py プロジェクト: amusecode/amuse
def new_single_star(mass, pos, vel):
    single_star = Particle()
    single_star.mass = mass
    single_star.position = pos
    single_star.velocity = vel
    single_star.radius = 1.0 | units.RSun
    return single_star
コード例 #4
0
    def result(self):
        if self.pickle_file is None:
            self.retrieve_stellar_structure()
        else:
            self.unpickle_stellar_structure()

        if self.with_core_particle:
            self.setup_core_parameters()

        sph_particles = self.convert_to_SPH()
        if self.do_relax:
            for result_string in self.relax(sph_particles):
                print(result_string)

        specific_internal_energy, composition, mu = self.interpolate_internal_energy(
            sph_particles.position.lengths(),
            do_composition_too = self.do_store_composition
        )
        sph_particles.u = specific_internal_energy
        if self.do_store_composition:
            sph_particles.add_vector_attribute("composition", self.species_names)
            sph_particles.composition = composition
            sph_particles.mu = mu

        if self.with_core_particle and self.core_radius:
            core_particle = Particle()
            core_particle.mass = self.core_mass
            core_particle.position = [0.0, 0.0, 0.0] | units.m
            core_particle.velocity = [0.0, 0.0, 0.0] | units.m / units.s
            core_particle.radius = self.core_radius
            return StellarModelInSPH(gas_particles=sph_particles, core_particle=core_particle, core_radius=self.core_radius)
        return StellarModelInSPH(gas_particles=sph_particles, core_particle=None, core_radius=None)
コード例 #5
0
def new_single_star(mass, pos, vel):
    single_star = Particle()
    single_star.mass = mass
    single_star.position = pos
    single_star.velocity = vel
    single_star.radius = 1.0 | units.RSun
    return single_star
コード例 #6
0
    def test12(self):
        N = 1000
        Lstar = 100 | units.LSun
        boxsize = 10 | units.parsec
        rho = 1.0 | (units.amu / units.cm**3)
        t_end = 0.01 | units.Myr
        internal_energy = (9. | units.kms)**2

        source = Particle()
        source.position = (0, 0, 0) | units.parsec
        source.flux = Lstar / (20. | units.eV)
        source.rho = rho
        source.xion = 0.0
        source.u = internal_energy

        ism = ism_cube(N, boxsize / 2., rho, internal_energy).result
        ism.rho = rho
        ism.flux = 0. | units.s**-1
        ism.xion = source.xion

        radiative = SimpleX()
        radiative.parameters.box_size = 1.001 * boxsize
        radiative.parameters.timestep = 0.001 | units.Myr

        radiative.particles.add_particle(source)
        radiative.particles.add_particles(ism)

        radiative.evolve_model(t_end)
        self.assertAlmostRelativeEquals(0.0750819123073,
                                        radiative.particles.xion.mean(), 1)
        radiative.stop()
コード例 #7
0
    def test7(self):
        print "Testing Pikachu states"
        stars = new_plummer_model(100)
        black_hole = Particle()
        black_hole.mass = 1.0 | nbody_system.mass
        black_hole.radius = 0.0 | nbody_system.length
        black_hole.position = [0.0, 0.0, 0.0] | nbody_system.length
        black_hole.velocity = [0.0, 0.0, 0.0] | nbody_system.speed

        print "First do everything manually:"
        instance = self.new_instance_of_an_optional_code(
            Pikachu, **default_options)
        self.assertEquals(instance.get_name_of_current_state(),
                          'UNINITIALIZED')
        instance.initialize_code()
        self.assertEquals(instance.get_name_of_current_state(), 'INITIALIZED')
        #~        instance.parameters.rcut_out_star_star = 1.0 | nbody_system.length
        instance.parameters.timestep = 0.001 | nbody_system.time
        instance.commit_parameters()
        self.assertEquals(instance.get_name_of_current_state(), 'EDIT')
        instance.particles.add_particles(stars)
        instance.commit_particles()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.particles.remove_particle(stars[0])
        instance.particles.add_particle(black_hole)
        self.assertEquals(instance.get_name_of_current_state(), 'UPDATE')
        instance.recommit_particles()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.evolve_model(0.001 | nbody_system.time)
        self.assertEquals(instance.get_name_of_current_state(), 'EVOLVED')
        instance.synchronize_model()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.cleanup_code()
        self.assertEquals(instance.get_name_of_current_state(), 'END')
        instance.stop()

        print "initialize_code(), commit_parameters(), (re)commit_particles(), " \
            "synchronize_model(), and cleanup_code() should be called " \
            "automatically before editing parameters, new_particle(), get_xx(), and stop():"
        instance = self.new_instance_of_an_optional_code(
            Pikachu, **default_options)
        self.assertEquals(instance.get_name_of_current_state(),
                          'UNINITIALIZED')
        instance.parameters.timestep = 0.001 | nbody_system.time
        self.assertEquals(instance.get_name_of_current_state(), 'INITIALIZED')
        instance.particles.add_particles(stars)
        self.assertEquals(instance.get_name_of_current_state(), 'EDIT')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.particles.remove_particle(stars[0])
        instance.particles.add_particle(black_hole)
        self.assertEquals(instance.get_name_of_current_state(), 'UPDATE')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.evolve_model(0.001 | nbody_system.time)
        self.assertEquals(instance.get_name_of_current_state(), 'EVOLVED')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.stop()
        self.assertEquals(instance.get_name_of_current_state(), 'STOPPED')
コード例 #8
0
ファイル: test_kepler.py プロジェクト: yon23/amuse-framework
def test_kepler(N=10000, tend=1.| units.yr,method=0):

  numpy.random.seed(12345)

  conv=nbody_system.nbody_to_si(2.| units.MSun, 5.|units.AU)

  comets=new_plummer_model(N,conv)

  sun=Particle(mass=1.|units.MSun)

  sun.position=[0,0,0]|units.AU
  sun.velocity=[0,0,0]|units.kms

  comets.mass*=0.

  code=Kepler(conv,redirection="none")

  code.set_method(method)

  code.central_particle.add_particle(sun)
  code.orbiters.add_particles(comets)

  a0,eps0=elements(sun.mass,code.orbiters.x,code.orbiters.y,code.orbiters.z,
                     code.orbiters.vx,code.orbiters.vy,code.orbiters.vz)


#  print code.orbiters.x[0]
  print orbital_elements_from_binary(code.particles[0:2],constants.G)

  t1=time.time()
  code.evolve_model(tend)
  t2=time.time()

  print orbital_elements_from_binary(code.particles[0:2],constants.G)
#  print code.orbiters.x[0]



  a,eps=elements(sun.mass,code.orbiters.x,code.orbiters.y,code.orbiters.z,
                     code.orbiters.vx,code.orbiters.vy,code.orbiters.vz)

  da=abs((a-a0)/a0)
  deps=abs(eps-eps0)/eps0

  dev=numpy.where(da > 0.00001)[0]
  print len(dev)

  print a0[dev].value_in(units.AU)
  print eps0[dev]

#  pyplot.plot(a0[dev].value_in(units.AU),eps0[dev],"ro")
#  pyplot.plot(a[dev].value_in(units.AU),eps[dev],"g+")

  print "max da,deps:",da.max(), deps.max()

  print "time:",t2-t1

#  pyplot.show()

  return t2-t1,da.max(),deps.max()
コード例 #9
0
ファイル: merge_recipes.py プロジェクト: rieder/ekster
def form_new_star(
    densest_gas_particle,
    gas_particles,
    # density_threshold=
):
    """
    Forms a new star by merging all gas particles within a Jeans radius of the
    densest particle. Returns the new star and all particles used to make it.
    """
    new_star = Particle()
    gas_copy = gas_particles.copy()

    # densest_gas_particle = gas_copy.sorted_by_attribute("density")[0]
    jeans_radius = 0.025 | units.parsec  # 100 | units.AU
    gas_copy.position -= densest_gas_particle.position
    gas_copy.distance_to_core = gas_copy.position.lengths()
    dense_gas = gas_copy.select(lambda x: x < jeans_radius,
                                ["distance_to_core"])
    new_star.mass = dense_gas.mass.sum()
    new_star.position = (dense_gas.center_of_mass() +
                         densest_gas_particle.position)
    new_star.velocity = dense_gas.center_of_mass_velocity()
    new_star.radius = jeans_radius
    absorbed_gas = dense_gas

    return new_star, absorbed_gas
コード例 #10
0
ファイル: test_simplex.py プロジェクト: stevemcmillan/amuse
    def test12(self):
        N = 1000
        Lstar=100|units.LSun
        boxsize=10|units.parsec
        rho=1.0 | (units.amu/units.cm**3)
        t_end=0.01 |units.Myr
        internal_energy = (9. |units.kms)**2

        source=Particle()
        source.position = (0, 0, 0) |units.parsec
        source.flux = Lstar/(20. | units.eV)
        source.rho = rho
        source.xion = 0.0
        source.u = internal_energy

        ism = ism_cube(N, boxsize/2., rho, internal_energy).result
        ism.rho = rho
        ism.flux = 0. | units.s**-1
        ism.xion = source.xion

        radiative = SimpleX()
        radiative.parameters.box_size=1.001*boxsize    
        radiative.parameters.timestep=0.001 | units.Myr

        radiative.particles.add_particle(source)
        radiative.particles.add_particles(ism)

        radiative.evolve_model(t_end)
        self.assertAlmostRelativeEquals( 0.0750819123073, radiative.particles.xion.mean(), 1)
        radiative.stop()
コード例 #11
0
ファイル: XiTau.py プロジェクト: sarasally/amuse
def continue_evolution(sph_code, dynamics_code, t_end, n_steps, 
        relaxed_giant_output_base_name, do_energy_evolution_plot):
    print("Loading snapshots...", end=' ')
    files = os.listdir("snapshots")
    files.sort()
    files = files[-4:]
    print(files)
    binary = read_set_from_file(os.path.join("snapshots", files[0]), format='amuse')
    gd_particles = read_set_from_file(os.path.join("snapshots", files[1]), format='amuse')
    sph_particles = read_set_from_file(os.path.join("snapshots", files[2]), format='amuse')
    
    snapshotfile = os.path.join("..", "giant_models", relaxed_giant_output_base_name + "_core.amuse")
    core_particle = read_set_from_file(snapshotfile, format='amuse')
    
    giant_model = StellarModelInSPH(
        gas_particles = sph_particles, 
        core_particle = gd_particles[0], 
        core_radius = core_particle.radius)
    
    view_on_giant = Particle()
    view_on_giant.position = [0]*3 | units.m
    view_on_giant.velocity = [0]*3 | units.m / units.s
    
    print("\nSetting up {0} to simulate inner binary system".format(dynamics_code.__name__))
    binary_system = prepare_binary_system(dynamics_code, binary)
    
    print("\nSetting up {0} to simulate giant in SPH".format(sph_code.__name__))
    giant_system = prepare_giant_system(sph_code, giant_model, view_on_giant, t_end, n_steps)
    
    print("\nEvolving with bridge between", sph_code.__name__, "and", dynamics_code.__name__)
    evolve_coupled_system(binary_system, giant_system, t_end, n_steps, do_energy_evolution_plot, 
        previous_data = os.path.join("snapshots", files[3]))
    print("Done")
コード例 #12
0
def new_particle_from_cluster_core(particles,
                                   unit_converter=None,
                                   density_weighting_power=2,
                                   cm=None,
                                   reuse_hop=False,
                                   hop=HopContainer()):
    """
    Uses Hop to find the density centre (core) of a particle distribution
    and stores the properties of this core on a particle:
    position, velocity, (core) radius and (core) density.
    
    Particles are assigned weights that depend on the density (as determined by 
    Hop) to a certain power.
    The default weighting power is 2, which is most commonly used. Set 
    density_weighting_power to 1 in order to get the original weighting of 
    Casertano & Hut (1985, ApJ, 298, 80).
    
    :argument unit_converter: Required if the particles are in SI units
    :argument density_weighting_power: Particle properties are weighted by density to this power
    """
    if isinstance(hop, HopContainer):
        hop.initialize(unit_converter)
        hop = hop.code
    in_hop = hop.particles.add_particles(particles)
    hop.parameters.density_method = 2
    hop.parameters.number_of_neighbors_for_local_density = 7
    hop.calculate_densities()
    density = in_hop.density.copy()
    if not reuse_hop:
        hop.stop()

    weights = (density**density_weighting_power).reshape((-1, 1))
    # Reshape makes sure that density can be multiplied with vectors, e.g. position

    result = Particle()
    result.density = density.amax()
    total_weight = weights.sum()
    if cm is None:
        result.position = (weights *
                           particles.position).sum(axis=0) / total_weight
    else:
        result.position = cm
    result.velocity = (weights * particles.velocity).sum(axis=0) / total_weight
    result.radius = (
        weights.flatten() *
        (particles.position - result.position).lengths()).sum() / total_weight
    return result
コード例 #13
0
ファイル: test_pikachu.py プロジェクト: Ingwar/amuse
    def test7(self):
        print "Testing Pikachu states"
        stars = new_plummer_model(100)
        black_hole = Particle()
        black_hole.mass = 1.0 | nbody_system.mass
        black_hole.radius =  0.0 | nbody_system.length
        black_hole.position = [0.0, 0.0, 0.0] | nbody_system.length
        black_hole.velocity = [0.0, 0.0, 0.0] | nbody_system.speed
        
        print "First do everything manually:"
        instance = self.new_instance_of_an_optional_code(Pikachu, **default_options)
        self.assertEquals(instance.get_name_of_current_state(), 'UNINITIALIZED')
        instance.initialize_code()
        self.assertEquals(instance.get_name_of_current_state(), 'INITIALIZED')
#~        instance.parameters.rcut_out_star_star = 1.0 | nbody_system.length
        instance.parameters.timestep = 0.001 | nbody_system.time
        instance.commit_parameters()
        self.assertEquals(instance.get_name_of_current_state(), 'EDIT')
        instance.particles.add_particles(stars)
        instance.commit_particles()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.particles.remove_particle(stars[0])
        instance.particles.add_particle(black_hole)
        self.assertEquals(instance.get_name_of_current_state(), 'UPDATE')
        instance.recommit_particles()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.evolve_model(0.001 | nbody_system.time)
        self.assertEquals(instance.get_name_of_current_state(), 'EVOLVED')
        instance.synchronize_model()
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.cleanup_code()
        self.assertEquals(instance.get_name_of_current_state(), 'END')
        instance.stop()
        
        print "initialize_code(), commit_parameters(), (re)commit_particles(), " \
            "synchronize_model(), and cleanup_code() should be called " \
            "automatically before editing parameters, new_particle(), get_xx(), and stop():"
        instance = self.new_instance_of_an_optional_code(Pikachu, **default_options)
        self.assertEquals(instance.get_name_of_current_state(), 'UNINITIALIZED')
        instance.parameters.timestep = 0.001 | nbody_system.time
        self.assertEquals(instance.get_name_of_current_state(), 'INITIALIZED')
        instance.particles.add_particles(stars)
        self.assertEquals(instance.get_name_of_current_state(), 'EDIT')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.particles.remove_particle(stars[0])
        instance.particles.add_particle(black_hole)
        self.assertEquals(instance.get_name_of_current_state(), 'UPDATE')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.evolve_model(0.001 | nbody_system.time)
        self.assertEquals(instance.get_name_of_current_state(), 'EVOLVED')
        mass = instance.particles[0].mass
        self.assertEquals(instance.get_name_of_current_state(), 'RUN')
        instance.stop()
        self.assertEquals(instance.get_name_of_current_state(), 'STOPPED')
コード例 #14
0
    def __init__(self, potential, particle=None):
        self.potential = potential

        if particle is None:
            particle = Particle()
            particle.position = [0., 0., 0.] | units.parsec
            particle.velocity = [0., 0., 0.] | units.kms

        self.particles = Particles()
        self.particles.add_particle(particle)
コード例 #15
0
ファイル: static_potentials.py プロジェクト: Ingwar/amuse
    def __init__(self, potential, particle=None):
        self.potential = potential

        if particle is None:
            particle = Particle()
            particle.position = [0., 0., 0.] | units.parsec
            particle.velocity = [0., 0., 0.] | units.kms

        self.particles = Particles()
        self.particles.add_particle(particle)
コード例 #16
0
ファイル: merge_recipes.py プロジェクト: rieder/ekster
def merge_two_stars(primary, secondary):
    "Merge two colliding stars into one new one"
    colliders = Particles()
    colliders.add_particle(primary)
    colliders.add_particle(secondary)
    new_particle = Particle()
    new_particle.mass = colliders.mass.sum()
    new_particle.position = colliders.center_of_mass()
    new_particle.velocity = colliders.center_of_mass_velocity()

    return new_particle
コード例 #17
0
ファイル: particle_attributes.py プロジェクト: rieder/amuse
def new_particle_from_cluster_core(
    particles, unit_converter=None, density_weighting_power=2, cm=None, reuse_hop=False, hop=HopContainer()
):
    """
    Uses Hop to find the density centre (core) of a particle distribution
    and stores the properties of this core on a particle:
    position, velocity, (core) radius and (core) density.
    
    Particles are assigned weights that depend on the density (as determined by 
    Hop) to a certain power.
    The default weighting power is 2, which is most commonly used. Set 
    density_weighting_power to 1 in order to get the original weighting of 
    Casertano & Hut (1985, ApJ, 298, 80).
    
    :argument unit_converter: Required if the particles are in SI units
    :argument density_weighting_power: Particle properties are weighted by density to this power
    """
    if isinstance(hop, HopContainer):
        hop.initialize(unit_converter)
        hop = hop.code
    in_hop = hop.particles.add_particles(particles)
    hop.parameters.density_method = 2
    hop.parameters.number_of_neighbors_for_local_density = 7
    hop.calculate_densities()
    density = in_hop.density.copy()
    if not reuse_hop:
        hop.stop()

    weights = (density ** density_weighting_power).reshape((-1, 1))
    # Reshape makes sure that density can be multiplied with vectors, e.g. position

    result = Particle()
    result.density = density.amax()
    total_weight = weights.sum()
    if cm is None:
        result.position = (weights * particles.position).sum(axis=0) / total_weight
    else:
        result.position = cm
    result.velocity = (weights * particles.velocity).sum(axis=0) / total_weight
    result.radius = (weights.flatten() * (particles.position - result.position).lengths()).sum() / total_weight
    return result
コード例 #18
0
ファイル: XiTau.py プロジェクト: amusecode/amuse
def set_up_outer_star(inner_binary_mass):
    semimajor_axis = 1.22726535008 | units.AU
    eccentricity = 0.15
    inclination = math.radians(9.0)
    
    print "   Initializing outer star"
    giant = Particle()
    giant.mass = 5.5 | units.MSun
    giant.position = semimajor_axis * ([math.cos(inclination), 0, math.sin(inclination)] | units.none)
    giant.velocity = get_relative_velocity(giant.mass + inner_binary_mass, 
        semimajor_axis, eccentricity) * ([0, 1, 0] | units.none)
    return giant
コード例 #19
0
def set_up_outer_star(inner_binary_mass):
    semimajor_axis = triple_parameters["a_out"]
    eccentricity = triple_parameters["eccentricity_out"]
    print "   Initializing outer star"
    giant = Particle()
    giant.mass = triple_parameters["mass_out"]
    giant.position = semimajor_axis * (1 + eccentricity) * ([1, 0, 0]
                                                            | units.none)
    giant.velocity = get_relative_velocity_at_apastron(
        giant.mass + inner_binary_mass, semimajor_axis,
        eccentricity) * ([0, 1, 0] | units.none)
    return giant
コード例 #20
0
ファイル: XiTau.py プロジェクト: sarasally/amuse
def set_up_outer_star(inner_binary_mass):
    semimajor_axis = 1.22726535008 | units.AU
    eccentricity = 0.15
    inclination = math.radians(9.0)
    
    print("   Initializing outer star")
    giant = Particle()
    giant.mass = 5.5 | units.MSun
    giant.position = semimajor_axis * ([math.cos(inclination), 0, math.sin(inclination)] | units.none)
    giant.velocity = get_relative_velocity(giant.mass + inner_binary_mass, 
        semimajor_axis, eccentricity) * ([0, 1, 0] | units.none)
    return giant
コード例 #21
0
ファイル: test_fastkick.py プロジェクト: Ingwar/amuse
 def test1(self):
     print "Testing FastKick (SI)"
     sun = Particle()
     sun.mass = 1.0|units.MSun
     sun.position = [0, 0, 0] | units.m
     convert_nbody = nbody_system.nbody_to_si(1.0 | units.MSun, 1.0 | units.AU)
     fastkick = self.new_fastkick_instance(convert_nbody)
     fastkick.particles.add_particle(sun)
     ax, ay, az = fastkick.get_gravity_at_point(0|units.AU, 1|units.AU, 0|units.AU, 0|units.AU)
     fastkick.stop()
     self.assertAlmostRelativeEqual(ax, -4*math.pi**2 | units.AU / units.yr**2, 3)
     self.assertAlmostRelativeEqual(ay, 0 | units.m * units.s**-2, 6)
     self.assertAlmostRelativeEqual(az, 0 | units.m * units.s**-2, 6)
コード例 #22
0
def setup_system():
    """
        Galacitic center potential and Arches cluster
        position from Kruijssen 2014
    """
    potential = static_potentials.Galactic_Center_Potential_Kruijssen()
    cluster = Particle()

    # At time 2.05 in KDL15
    cluster.position = [-17.55767, -53.26560, -9.39921] | units.parsec
    cluster.velocity = [-187.68008, 80.45276, 33.96556] | units.kms

    cluster.position += coordinate_correction
    return potential, cluster
コード例 #23
0
def setup_system():
    """
        Galacitic center potential and Arches cluster
        position from Kruijssen 2014
    """
    potential = static_potentials.Galactic_Center_Potential_Kruijssen()
    cluster = Particle()

    # At time 2.05 in KDL15
    cluster.position = [-17.55767, -53.26560, -9.39921] | units.parsec
    cluster.velocity = [-187.68008, 80.45276, 33.96556] | units.kms

    cluster.position += coordinate_correction
    return potential, cluster
コード例 #24
0
def new_system(star_mass=1 | units.MSun,
               star_radius=1 | units.RSun,
               disk_minimum_radius=0.05 | units.AU,
               disk_maximum_radius=10 | units.AU,
               disk_mass=20 | MEarth,
               accurancy=0.0001,
               planet_density=3 | units.g / units.cm**3,
               rng=None,
               kepler=None):

    central_particle = Particle()
    central_particle.mass = star_mass
    central_particle.position = (0, 0, 0) | units.AU
    central_particle.velocity = (0, 0, 0) | units.kms
    central_particle.radius = star_radius
    central_particle.name = "star"
    central_particle.type = "star"
    central_particle.id = 0

    if rng is None:
        rng = numpy.random

    converter = nbody_system.nbody_to_si(1 | units.MSun, 1 | units.AU)

    if kepler is None:
        kepler = Kepler(converter)
        kepler.initialize_code()

    m, r, f = new_planet_distribution(disk_minimum_radius, disk_maximum_radius,
                                      disk_mass, accurancy)

    planets = make_planets(central_particle,
                           m,
                           r,
                           density=planet_density,
                           phi=0,
                           theta=None,
                           kepler=kepler,
                           rng=rng)
    planets.name = "planet"
    planets.type = "planet"
    for i in range(len(planets)):
        planets[i].id = i

    central_particle.planets = planets
    kepler.stop()
    p = Particles()
    p.add_particle(central_particle)
    return p
def get_moons_for_planet(planet, delta_JD=0. | units.day):
    """
  The Earth's moon
  as for JD = 2457099.500000000 = A.D. 2015-Mar-18 00:00:00.0000 (CT)
  https://ssd.jpl.nasa.gov/?sat_elem
  """

    data = numpy.array([tuple(entry) for entry in _lunar_data],
                       dtype=[('planet_name', 'S10'), ('name', 'S10'),
                              ('mass', '<f8'), ('radius', '<f8'),
                              ('semimajor_axis', '<f8'),
                              ('eccentricity', '<f8'),
                              ('argument_of_peri', '<f8'),
                              ('mean_anomaly', '<f8'), ('inclination', '<f8'),
                              ('longitude_oan', '<f8')])
    moon_data = data[data['planet_name'] == planet.name.encode('UTF-8')]
    print("Planet=", planet.name, "moon=", moon_data["name"])
    moons = Particles()
    if len(moon_data["name"]):
        print(len(moon_data["name"]))
        for moon in moon_data:
            #Ignore the moon for now, because it's complicated
            if planet.name == "EarthMoon":
                planet.mass -= moon["mass"] * 1.e+16 | units.kg
                planet.name = "Earth"
            #print moon
            r, v = get_position(planet.mass,
                                moon["mass"] * 1.e+16 | units.kg,
                                moon["eccentricity"],
                                moon["semimajor_axis"] | units.km,
                                numpy.deg2rad(moon["mean_anomaly"]),
                                numpy.deg2rad(moon["inclination"]),
                                numpy.deg2rad(moon["longitude_oan"]),
                                numpy.deg2rad(moon["argument_of_peri"]),
                                delta_t=delta_JD)
            single_moon = Particle()
            single_moon.type = "moon"
            single_moon.name = moon["name"]
            single_moon.mass = moon["mass"] * 1.e+16 | units.kg
            single_moon.hostname = moon["planet_name"]
            single_moon.radius = moon["radius"] | units.km
            single_moon.position = r
            single_moon.position += planet.position
            single_moon.velocity = v
            single_moon.velocity += planet.velocity
            moons.add_particle(single_moon)

    return moons
コード例 #26
0
 def test1(self):
     print("Testing FastKick (SI)")
     sun = Particle()
     sun.mass = 1.0 | units.MSun
     sun.position = [0, 0, 0] | units.m
     convert_nbody = nbody_system.nbody_to_si(1.0 | units.MSun,
                                              1.0 | units.AU)
     fastkick = self.new_fastkick_instance(convert_nbody)
     fastkick.particles.add_particle(sun)
     ax, ay, az = fastkick.get_gravity_at_point(0 | units.AU, 1 | units.AU,
                                                0 | units.AU, 0 | units.AU)
     fastkick.stop()
     self.assertAlmostRelativeEqual(
         ax, -4 * math.pi**2 | units.AU / units.yr**2, 3)
     self.assertAlmostRelativeEqual(ay, 0 | units.m * units.s**-2, 6)
     self.assertAlmostRelativeEqual(az, 0 | units.m * units.s**-2, 6)
コード例 #27
0
def new_system(
        star_mass = 1|units.MSun, 
        star_radius = 1|units.RSun, 
        disk_minumum_radius = 0.05 | units.AU,
        disk_maximum_radius = 10 | units.AU,
        disk_mass = 20 | MEarth,
        accurancy = 0.0001, 
        planet_density =  3 | units.g/units.cm**3,
        rng = None,
        kepler = None):
            
    central_particle = Particle()
    central_particle.mass =  star_mass
    central_particle.position = (0,0,0) | units.AU
    central_particle.velocity = (0,0,0) | units.kms
    central_particle.radius = star_radius
    
    if rng is None:
        rng = numpy.random
        
    converter = nbody_system.nbody_to_si(1|units.MSun, 1 | units.AU)
    
    if kepler is None:
        kepler = Kepler(converter)
        kepler.initialize_code()
        
    m, r, f = new_planet_distribution(
        disk_minumum_radius, disk_maximum_radius, 
        disk_mass,
        accurancy
    )
    
    planets = make_planets(
        central_particle, 
        m, r, 
        density = planet_density, 
        phi = 0, theta = None, 
        kepler = kepler, 
        rng = rng
    )
    
    central_particle.planets = planets
    kepler.stop()
    p = Particles()
    p.add_particle(central_particle)
    return p
コード例 #28
0
def set_up_outer_star(inner_binary_mass):
    orbital_period = 4020.0 | units.day
    mass = 1.3 | units.MSun
    semimajor_axis = (((constants.G *
                        (inner_binary_mass + mass) * orbital_period**2) /
                       (4 * numpy.pi**2))**(1.0 / 3.0)).as_quantity_in(
                           units.RSun)

    print "   Initializing outer star"
    print "   Semimajor axis outer binary:", semimajor_axis
    giant = Particle()
    giant.mass = mass
    giant.position = semimajor_axis * ([1, 0, 0] | units.none)
    giant.velocity = get_relative_velocity(giant.mass + inner_binary_mass,
                                           semimajor_axis,
                                           0) * ([0, 1, 0] | units.none)
    return giant
コード例 #29
0
def nbody_integrator(Ncl, mcl, rcl, t_end, n_steps, escape_velocity_fraction,
                     R):
    converter = nbody_system.nbody_to_si(mcl, rcl)
    bodies = new_plummer_model(Ncl, convert_nbody=converter)

    #estimate of milky way mass by "Mass models of the Milky Way", McMillan
    blackhole_mass = 1.26e12 | units.MSun
    blackhole = Particle(mass=blackhole_mass)
    blackhole.position = [0, 0, 0] | units.m

    cluster_velocity = [0, 0, 0] | units.m / units.s
    cluster_position = [0, 0, 0] | units.parsec
    cluster_position[0] = R
    G_si = converter.to_si(nbody_system.G)
    escape_v = (2 * G_si * blackhole_mass / R).sqrt().as_quantity_in(units.m /
                                                                     units.s)
    V = escape_v * escape_velocity_fraction
    cluster_velocity[1] = V
    bodies.move_to_center()
    bodies.velocity += cluster_velocity
    bodies.position += cluster_position
    bodies.add_particle(blackhole)

    gravity = BHTree(converter)
    gravity.particles.add_particles(bodies)
    channel_from_gravity_to_framework = gravity.particles.\
        new_channel_to(bodies)

    time = zero
    dt = t_end / float(n_steps)
    x = 0
    base_path = "encounter_plots/"+str(R.value_in(units.parsec))+"_"+\
        str(escape_velocity_fraction)+"_"
    while time < t_end:
        plot_cluster(bodies, base_path + str(x), time, rcl, V)
        time += dt
        gravity.evolve_model(time)
        channel_from_gravity_to_framework.copy()
        x += 1
    plot_cluster(bodies, base_path + str(x), time, rcl, V)

    gravity.stop()
    return V, bodies
コード例 #30
0
def nbody_integrator(Ncl, mcl, rcl, t_end, n_steps, escape_velocity_fraction, R):
    converter = nbody_system.nbody_to_si(mcl, rcl)
    bodies = new_plummer_model(Ncl, convert_nbody=converter)

    #estimate of milky way mass by "Mass models of the Milky Way", McMillan
    blackhole_mass = 1.26e12 | units.MSun
    blackhole = Particle(mass=blackhole_mass)
    blackhole.position = [0,0,0] | units.m

    cluster_velocity = [0,0,0] | units.m / units.s
    cluster_position = [0,0,0] | units.parsec
    cluster_position[0] = R
    G_si = converter.to_si(nbody_system.G)
    escape_v = (2*G_si*blackhole_mass/R).sqrt().as_quantity_in(units.m/units.s)
    V = escape_v * escape_velocity_fraction
    cluster_velocity[1] = V
    bodies.move_to_center()
    bodies.velocity += cluster_velocity
    bodies.position += cluster_position
    bodies.add_particle(blackhole)
        

    gravity = BHTree(converter)
    gravity.particles.add_particles(bodies)
    channel_from_gravity_to_framework = gravity.particles.\
        new_channel_to(bodies)

    time = zero
    dt = t_end / float(n_steps)
    x = 0
    base_path = "encounter_plots/"+str(R.value_in(units.parsec))+"_"+\
        str(escape_velocity_fraction)+"_"
    while time < t_end:
        plot_cluster(bodies, base_path+str(x),time, rcl, V)
        time += dt
        gravity.evolve_model(time)
        channel_from_gravity_to_framework.copy()
        x+=1
    plot_cluster(bodies, base_path+str(x),time, rcl, V)

    gravity.stop()
    return V, bodies
コード例 #31
0
def get_moons_for_planet(planet, delta_JD=0.|units.day):
  """
  The Earth's moon
  as for JD = 2457099.500000000 = A.D. 2015-Mar-18 00:00:00.0000 (CT)
  https://ssd.jpl.nasa.gov/?sat_elem
  """

  data = numpy.array([tuple(entry) for entry in _lunar_data],
        dtype=[('planet_name','S10'), ('name','S10'), 
        ('mass','<f8'), ('radius','<f8'), ('semimajor_axis','<f8'), 
        ('eccentricity','<f8'), ('argument_of_peri','<f8'),
        ('mean_anomaly','<f8'), ('inclination','<f8'), ('longitude_oan','<f8')])
  moon_data = data[data['planet_name']==planet.name]
  print "Planet=", planet.name, "moon=", moon_data["name"]
  moons = Particles()
  if len(moon_data["name"]):
      print len(moon_data["name"])
      for moon in moon_data:
          #print moon
          r, v = get_position(planet.mass,
                              moon["mass"] * 1.e+16 | units.kg,
                              moon["eccentricity"],
                              moon["semimajor_axis"]|units.km,
                              numpy.deg2rad(moon["mean_anomaly"]),
                              numpy.deg2rad(moon["inclination"]),
                              numpy.deg2rad(moon["longitude_oan"]),
                              numpy.deg2rad(moon["argument_of_peri"]),
                              delta_t=delta_JD)
          single_moon = Particle()
          single_moon.type = "moon"
          single_moon.name = moon["name"]
          single_moon.mass = moon["mass"] * 1.e+16 | units.kg
          single_moon.hostname = moon["planet_name"]
          single_moon.radius = moon["radius"] | units.km
          single_moon.position = r
          single_moon.position += planet.position
          single_moon.velocity = v
          single_moon.velocity += planet.velocity
          moons.add_particle(single_moon)
    
  return moons
コード例 #32
0
def giant_to_sph(giant, stellar_structure_file, number_of_sph_particles):
    model = convert_stellar_model_to_SPH(None,
                                         number_of_sph_particles,
                                         pickle_file=stellar_structure_file,
                                         with_core_particle=True,
                                         target_core_mass=2.0 | units.MSun,
                                         do_store_composition=False,
                                         base_grid_options=dict(type="fcc"))
    sph_giant = model.gas_particles
    if model.core_particle is None:
        core = Particle(mass=0 | units.MSun, radius=1 | units.RSun)
        core_radius = core.radius
    else:
        core = model.core_particle
        core_radius = model.core_radius
    sph_giant.position += giant.position
    sph_giant.velocity += giant.velocity
    core.position = giant.position
    core.velocity = giant.velocity
    print "Core radius:", core_radius.as_string_in(units.RSun)
    return sph_giant, core, core_radius
コード例 #33
0
def evolve_triple_with_wind(M1, M2, M3, Pora, Pin_0, ain_0, aout_0, ein_0,
                            eout_0, t_end, nsteps, scheme, dtse_fac):

    import random
    from amuse.ext.solarsystem import get_position

    time_framework = 0

    print "Initial masses:", M1, M2, M3
    t_stellar = 4.0 | units.Myr
    triple = Particles(3)
    triple[0].mass = M1
    triple[1].mass = M2
    triple[2].mass = M3
    stellar = SeBa()
    stellar.particles.add_particles(triple)
    channel_from_stellar = stellar.particles.new_channel_to(triple)
    t0 = ctime.time()
    stellar.evolve_model(t_stellar)
    delta_t = ctime.time() - t0
    time_framework += delta_t
    channel_from_stellar.copy_attributes(["mass"])
    M1 = triple[0].mass
    M2 = triple[1].mass
    M3 = triple[2].mass
    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Masses at time T:", M1, M2, M3

    # Inner binary

    tmp_stars = Particles(2)
    tmp_stars[0].mass = M1
    tmp_stars[1].mass = M2

    if Pora == 1:
        ain_0 = semimajor_axis(Pin_0, M1 + M2)
    else:
        Pin_0 = orbital_period(ain_0, M1 + M2)

    print 'ain_0 =', ain_0
    print 'M1+M2 =', M1 + M2
    print 'Pin_0 =', Pin_0.value_in(units.day), '[day]'
    #print 'semi:', semimajor_axis(Pin_0, M1+M2).value_in(units.AU), 'AU'
    #print 'period:', orbital_period(ain_0, M1+M2).value_in(units.day), '[day]'

    dt = 0.1 * Pin_0
    ma = 180
    inc = 30
    aop = 180
    lon = 0
    r, v = get_position(M1, M2, ein_0, ain_0, ma, inc, aop, lon, dt)
    tmp_stars[1].position = r
    tmp_stars[1].velocity = v
    tmp_stars.move_to_center()

    # Outer binary

    r, v = get_position(M1 + M2, M3, eout_0, aout_0, 0, 0, 0, 0, dt)
    tertiary = Particle()
    tertiary.mass = M3
    tertiary.position = r
    tertiary.velocity = v
    tmp_stars.add_particle(tertiary)
    tmp_stars.move_to_center()

    triple.position = tmp_stars.position
    triple.velocity = tmp_stars.velocity

    Mtriple = triple.mass.sum()
    Pout = orbital_period(aout_0, Mtriple)

    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Pout=", Pout.in_(units.Myr)

    converter = nbody_system.nbody_to_si(triple.mass.sum(), aout_0)
    gravity = Huayno(converter)
    gravity.particles.add_particles(triple)

    channel_from_framework_to_gd = triple.new_channel_to(gravity.particles)
    channel_from_gd_to_framework = gravity.particles.new_channel_to(triple)

    Etot_init = gravity.kinetic_energy + gravity.potential_energy
    Etot_prev = Etot_init

    gravity.particles.move_to_center()

    time = 0.0 | t_end.unit
    ts = t_stellar + time  # begin when stars have formed after 4.0 Myr years

    ain, ein, aout, eout, iin, iout = get_orbital_elements_of_triple(triple)
    print "Triple elements t=",  time,  \
        "inner:", triple[0].mass, triple[1].mass, ain, ein, iin, \
        "outer:", triple[2].mass, aout, eout, iout

    dt_diag = t_end / float(
        nsteps)  # how often we want to save the generated data
    t_diag = dt_diag

    t = [time.value_in(units.Myr)]
    smai = [ain / ain_0]
    ecci = [ein / ein_0]
    smao = [aout / aout_0]
    ecco = [eout / eout_0]
    inci = [iin]
    inco = [iout]
    ain = ain_0

    def advance_stellar(ts, dt):
        E0 = gravity.kinetic_energy + gravity.potential_energy
        ts += dt
        stellar.evolve_model(ts)
        channel_from_stellar.copy_attributes(["mass"])
        channel_from_framework_to_gd.copy_attributes(["mass"])
        return ts, gravity.kinetic_energy + gravity.potential_energy - E0

    def advance_stellar_with_massloss(
        ts,
        time_framework,
        dt_massloss=15e-9 | units.Myr,
        max_massloss=3e-4
        | units.MSun):  # Scheme 3: dt 8*10^-7, dm = 2*10^-5 (

        max_massloss = 0.0 | units.MSun  # massloss over full gravtiational time step  massloss0
        #max_massloss= 3e-6 | units.MSun # massloss over full gravtiational time step massloss1
        #max_massloss= 1e-6 | units.MSun # massloss over full gravtiational time step massloss2

        E0 = gravity.kinetic_energy + gravity.potential_energy
        massloss = -1 | units.MSun
        mass_0 = numpy.sum(stellar.particles.mass)
        dt_stellar = 0 | units.Myr
        niter = 0
        while massloss < max_massloss:
            ts += dt_massloss
            dt_stellar += dt_massloss  # counter for full time
            niter += 1
            t0 = ctime.time()
            stellar.evolve_model(ts)
            delta_t = ctime.time() - t0
            time_framework += delta_t
            massloss = 2. * (
                mass_0 - numpy.sum(stellar.particles.mass)
            )  # massloss over full gravtiational time step is x2

        channel_from_stellar.copy_attributes(["mass"])
        channel_from_framework_to_gd.copy_attributes(["mass"])

        print 'Tstellar:', dt_stellar, ', Total Mloss:', massloss, ' Niter:', niter

        return ts, time_framework, gravity.kinetic_energy + gravity.potential_energy - E0, dt_stellar

    def advance_gravity(tg, dt):
        tg += dt
        gravity.evolve_model(tg)
        channel_from_gd_to_framework.copy()
        return tg

    global_time = []
    global_massloss = []
    global_dmdt = []
    while time < t_end:

        Pin = orbital_period(ain, triple[0].mass + triple[1].mass)
        dt = dtse_fac * Pin
        dt *= random.random(
        )  # time step is chosen random between 0 and 50*Pin

        if scheme == 1:

            ts, dE_se = advance_stellar(ts, dt)
            time = advance_gravity(time, dt)

        elif scheme == 2:

            time = advance_gravity(time, dt)
            ts, dE_se = advance_stellar(ts, dt)

        elif scheme == 3:

            # inital mass
            mass_init = stellar.particles.mass.sum()

            # perform step
            ts, dE_se = advance_stellar(ts, dt / 2)
            time = advance_gravity(time, dt)
            ts, dE = advance_stellar(ts, dt / 2)
            dE_se += dE

            # add right vlaues
            global_time = numpy.append(global_time, time.value_in(units.Myr))
            global_massloss = numpy.append(
                global_massloss,
                mass_init.value_in(units.MSun) -
                numpy.sum(stellar.particles.mass).value_in(units.MSun))

        else:  # our scheme is 4

            # inital mass
            mass_init = stellar.particles.mass.sum()
            time_init = time.value_in(units.Myr) | units.Myr

            # get optimal dt to perform a time step without losing too much mass
            ts, time_framework, dE_se, dt_stellar = advance_stellar_with_massloss(
                ts, time_framework)

            # perform time step dt
            t0 = ctime.time()
            time = advance_gravity(time, dt_stellar * 2)
            ts, dE = advance_stellar(ts, dt_stellar)
            delta_t = ctime.time() - t0
            time_framework += delta_t
            dE_se += dE

            # save everything
            global_time = numpy.append(global_time, time.value_in(units.Myr))
            global_massloss = numpy.append(
                global_massloss,
                mass_init.value_in(units.MSun) -
                numpy.sum(stellar.particles.mass).value_in(units.MSun))
            global_dmdt = numpy.append(
                global_dmdt,
                (mass_init.value_in(units.MSun) -
                 numpy.sum(stellar.particles.mass).value_in(units.MSun)) /
                (time.value_in(units.Myr) - time_init.value_in(units.Myr)))

        if time >= t_diag:

            t_diag = time + dt_diag

            Ekin = gravity.kinetic_energy
            Epot = gravity.potential_energy
            Etot = Ekin + Epot
            dE = Etot_prev - Etot
            Mtot = triple.mass.sum()
            print "T=", time  #,
            #print "M=", Mtot, "(dM[SE]=", Mtot/Mtriple, ")",
            #print "E= ", Etot, "Q= ", Ekin/Epot,
            #print "dE=", (Etot_init-Etot)/Etot, "ddE=", (Etot_prev-Etot)/Etot,
            #print "(dE[SE]=", dE_se/Etot, ")"
            Etot_init -= dE
            Etot_prev = Etot
            ain, ein, aout, eout, iin, iout = get_orbital_elements_of_triple(
                triple)
            #print "Triple elements t=",  (4|units.Myr) + time,  \
            #    "inner:", triple[0].mass, triple[1].mass, ain, ein, \
            #    "outer:", triple[2].mass, aout, eout

            t.append(time.value_in(units.Myr))
            smai.append(ain / ain_0)
            ecci.append(ein / ein_0)
            smao.append(aout / aout_0)
            ecco.append(eout / eout_0)
            inci.append(iin)
            inco.append(iout)

            if eout > 1.0 or aout <= zero:
                print "Binary ionized or merged"
                break

    pyplot.close()

    data = numpy.array(zip(global_time, global_massloss, global_dmdt))
    numpy.save('massloss0', data)

    return t, smai, ecci, smao, ecco, inci, inco, time_framework
コード例 #34
0
def evolve_triple_with_wind(M1, M2, M3, Pora, Pin_0, ain_0, aout_0,
                            ein_0, eout_0, t_end, nsteps, scheme, integrator,
                            t_stellar, dt_se, dtse_fac, interp):

    import random
    from amuse.ext.solarsystem import get_position

    numpy.random.seed(42)

    print "Initial masses:", M1, M2, M3
    triple = Particles(3)
    triple[0].mass = M1
    triple[1].mass = M2
    triple[2].mass = M3
    stellar = SeBa()
    stellar.particles.add_particles(triple)
    channel_from_stellar = stellar.particles.new_channel_to(triple)

    # Evolve to t_stellar.
    
    stellar.evolve_model(t_stellar)
    channel_from_stellar.copy_attributes(["mass"])
    M1 = triple[0].mass
    M2 = triple[1].mass
    M3 = triple[2].mass
    print "t=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "R=", stellar.particles.radius.in_(units.RSun)
    print "L=", stellar.particles.luminosity.in_(units.LSun)
    print "T=", stellar.particles.temperature.in_(units.K)
    print "Mdot=", \
        -stellar.particles.wind_mass_loss_rate.in_(units.MSun/units.yr)

    # Start the dynamics.
    # Inner binary:
    
    tmp_stars = Particles(2)
    tmp_stars[0].mass = M1
    tmp_stars[1].mass = M2

    if Pora == 1:
        ain_0 = semimajor_axis(Pin_0, M1+M2)
    else:
        Pin_0 = orbital_period(ain_0, M1+M2)
    print 'Pin =', Pin_0
        
    print 'ain_0 =', ain_0
    print 'M1+M2 =', M1+M2
    print 'Pin_0 =', Pin_0.value_in(units.day), '[day]'
    #print 'semi:', semimajor_axis(Pin_0, M1+M2).value_in(units.AU), 'AU'
    #print 'period:', orbital_period(ain_0, M1+M2).value_in(units.day), '[day]'
    
    dt_init = 0.01*Pin_0
    ma = 180
    inc = 60
    aop = 180
    lon = 0
    r,v = get_position(M1, M2, ein_0, ain_0, ma, inc, aop, lon, dt_init)
    tmp_stars[1].position = r
    tmp_stars[1].velocity = v
    tmp_stars.move_to_center()

    # Outer binary:
    
    r,v = get_position(M1+M2, M3, eout_0, aout_0, 0, 0, 0, 0, dt_init)
    tertiary = Particle()
    tertiary.mass = M3
    tertiary.position = r
    tertiary.velocity = v
    tmp_stars.add_particle(tertiary)
    tmp_stars.move_to_center()

    triple.position = tmp_stars.position
    triple.velocity = tmp_stars.velocity

    Mtriple = triple.mass.sum()
    Pout = orbital_period(aout_0, Mtriple)

    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Pout=", Pout.in_(units.Myr)
    print 'tK =', ((M1+M2)/M3)*Pout**2*(1-eout_0**2)**1.5/Pin_0

    converter = nbody_system.nbody_to_si(triple.mass.sum(), aout_0)

    if integrator == 0:
        gravity = Hermite(converter)
        gravity.parameters.timestep_parameter = 0.01
    elif integrator == 1:
        gravity = SmallN(converter)
        gravity.parameters.timestep_parameter = 0.01
        gravity.parameters.full_unperturbed = 0
    elif integrator == 2:
        gravity = Huayno(converter)
        gravity.parameters.inttype_parameter = 20
        gravity.parameters.timestep = (1./256)*Pin_0
    else:
        gravity = symple(converter)
        gravity.parameters.integrator = 10
        #gravity.parameters.timestep_parameter = 0.
        gravity.parameters.timestep = (1./128)*Pin_0

    print gravity.parameters

    gravity.particles.add_particles(triple)
    channel_from_framework_to_gd = triple.new_channel_to(gravity.particles)
    channel_from_gd_to_framework = gravity.particles.new_channel_to(triple)
    
    Etot_init = gravity.kinetic_energy + gravity.potential_energy
    Etot_prev = Etot_init

    gravity.particles.move_to_center()

    # Note: time = t_diag = 0 at the start of the dynamical integration.
    
    dt_diag = t_end/float(nsteps)
    t_diag = dt_diag
    time = 0.0 | t_end.unit
    t_se = t_stellar + time

    print 't_end =', t_end
    print 'dt_diag =', dt_diag

    ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
    print "Triple elements t=",  time,  \
        "inner:", triple[0].mass, triple[1].mass, ain, ein, \
        "outer:", triple[2].mass, aout, eout

    t = [time.value_in(units.Myr)]
    Mtot = triple.mass.sum()
    mtot = [Mtot.value_in(units.MSun)]
    smai = [ain/ain_0] 
    ecci = [ein/ein_0]
    smao = [aout/aout_0] 
    ecco = [eout/eout_0]

    if interp:
        
        # Create arrays of stellar times and masses for interpolation.

        times = [time]
        masses = [triple.mass.copy()]
        while time < t_end:
            time += dt_se
            stellar.evolve_model(t_stellar+time)
            channel_from_stellar.copy_attributes(["mass"])
            times.append(time)
            masses.append(triple.mass.copy())

        time = 0.0 | t_end.unit
        print '\ntimes:', times, '\n'

    # Evolve the system.
    
    def advance_stellar(t_se, dt):
        E0 = gravity.kinetic_energy + gravity.potential_energy
        t_se += dt

        if interp:
            t = t_se-t_stellar
            i = int(t/dt_se)
            mass = masses[i] + (t-times[i])*(masses[i+1]-masses[i])/dt_se
            triple.mass = mass
            #print 't_se =', t_se, 'masses =', mass
        else:
            stellar.evolve_model(t_se)
            channel_from_stellar.copy_attributes(["mass"])

        channel_from_framework_to_gd.copy_attributes(["mass"])
        return t_se, gravity.kinetic_energy + gravity.potential_energy - E0

    def advance_gravity(tg, dt):
        tg += dt
        gravity.evolve_model(tg)
        channel_from_gd_to_framework.copy()
        return tg

    while time < t_end:

        if scheme == 1:

            # Advance to the next diagnostic time.
            
            dE_se = zero
            dt = t_diag - time

            if dt > 0|dt.unit:
                time = advance_gravity(time, dt)

        elif scheme == 2:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                t_se, dE_se = advance_stellar(t_se, dt)
                time = advance_gravity(time, dt)
            
        elif scheme == 3:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                time = advance_gravity(time, dt)
                t_se, dE_se = advance_stellar(t_se, dt)
            
        elif scheme == 4:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                t_se, dE_se = advance_stellar(t_se, 0.5*dt)
                time = advance_gravity(time, dt)
                t_se, dE_se2 = advance_stellar(t_se, 0.5*dt)
                dE_se += dE_se2
            
        elif scheme == 5:

            # Use the specified dt_se.
            
            dE_se = zero
            dt = dt_se
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:

                # For use with symple only: set up average mass loss.
    
                channel_from_stellar.copy_attributes(["mass"])
                m0 = triple.mass.copy()
                stellar.evolve_model(t_se+dt)
                channel_from_stellar.copy_attributes(["mass"])
                t_se = stellar.model_time
                m1 = triple.mass
                dmdt = (m1-m0)/dt
                for i in range(len(dmdt)):
                    gravity.set_dmdt(i, dmdt[i])

                time = advance_gravity(time, dt)

        else:

            print 'unknown option'
            sys.exit(0)

        if time >= t_diag:
            
            t_diag = time + dt_diag

            Ekin = gravity.kinetic_energy 
            Epot = gravity.potential_energy
            Etot = Ekin + Epot
            dE = Etot_prev - Etot
            Mtot = triple.mass.sum()
            print "T=", time, 
            print "M=", Mtot, "(dM[SE]=", Mtot/Mtriple, ")",
            print "E= ", Etot, "Q= ", Ekin/Epot,
            print "dE=", (Etot_init-Etot)/Etot, "ddE=", (Etot_prev-Etot)/Etot, 
            print "(dE[SE]=", dE_se/Etot, ")"
            Etot_init -= dE
            Etot_prev = Etot
            ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
            print "Triple elements t=",  t_stellar + time,  \
                "inner:", triple[0].mass, triple[1].mass, ain, ein, \
                "outer:", triple[2].mass, aout, eout

            t.append(time.value_in(units.yr))
            mtot.append(Mtot.value_in(units.MSun))
            smai.append(ain/ain_0)
            ecci.append(ein/ein_0)
            smao.append(aout/aout_0)
            ecco.append(eout/eout_0)

            if eout > 1 or aout <= zero:
                print "Binary ionized or merged"
                break

    gravity.stop()
    stellar.stop()

    return t, mtot, smai, ecci, smao, ecco
コード例 #35
0
ファイル: solarsystem.py プロジェクト: tjardaboekholt/amuse
def get_sun_and_planets(delta_JD=0.|units.day):
  """
  eight planets of the Solar System
  as for JD = 2457099.500000000 = A.D. 2015-Mar-18 00:00:00.0000 (CT)
  http://ssd.jpl.nasa.gov/horizons.cgi
  """
  planets = Particles(8)
  
  # mass
  planets.mass = [3.302e23,
                  48.685e23,
                  5.97219e24,
                  6.4185e23,
                  1898.13e24,
                  5.68319e26,
                  86.8103e24,
                  102.41e24] | units.kg
  
  # eccentricity
  planets_ecc = [2.056263501026885E-01,
                 6.756759719005901E-03,
                 1.715483324953308E-02,
                 9.347121362500883E-02,
                 4.877287772914470E-02,
                 5.429934603664216E-02,
                 4.911406962716518E-02,
                 8.494660388602767E-03]
  
  # semi-major axis
  planets_semi = [3.870989725156447E-01,
                  7.233252880006816E-01,
                  1.000816989613834E+00,
                  1.523624142457679E+00,
                  5.203543088590996E+00,
                  9.547316304899041E+00,
                  1.915982879739036E+01,
                  2.997013749028780E+01] | units.AU
  
  # mean anomaly [degrees]
  planets_mean_anomaly = [2.256667460183225E+02,
                          3.096834722926926E+02,
                          6.970055236286768E+01,
                          5.013506750245609E+01,
                          1.213203242081277E+02,
                          1.423311616732398E+02,
                          2.079860620353052E+02,
                          2.712246916734600E+02]
  planets_mean_anomaly = numpy.array(planets_mean_anomaly) * pi_over_180
  
  # inclination [IN degrees]
  planets_inclination = [7.004026765179669E+00,
                         3.394480103844425E+00,
                         3.563477431351056E-03,
                         1.848403408106458E+00,
                         1.303457729562742E+00,
                         2.488017444885577E+00,
                         7.728000142736371E-01,
                         1.767720502209091E+00]
  planets_inclination = numpy.array(planets_inclination) * pi_over_180
  
  # Longitude of Ascending Node [OM degrees]
  planets_longitude = [4.831163083479358E+01,
                       7.663982595051040E+01,
                       1.775515437672556E+02,
                       4.951282677064384E+01,
                       1.005036717671826E+02,
                       1.135683875842263E+02,
                       7.388411509910506E+01,
                       1.317497218434830E+02]
  planets_longitude = numpy.array(planets_longitude) * pi_over_180
  
  # Argument of Perihelion [W degrees]
  planets_argument = [2.916964171964058E+01,
                      5.469102797401222E+01,
                      2.877495001117996E+02,
                      2.865420083537150E+02,
                      2.740725976811202E+02,
                      3.398666856578898E+02,
                      9.666856264946740E+01,
                      2.951871807292030E+02]
  planets_argument = numpy.array(planets_argument) * pi_over_180
  
  planets.name = ['Mercury',
                  'Venus',
                  'Earth',
                  'Mars',
                  'Jupiter',
                  'Satrun',
                  'Uranus',
                  'Neptune']
  
  ### to compare with JPL, mass of the Sun needs to be rescaled
  #mg_nasa = 1.32712440018e20 | (units.m**3 / units.s**2)
  #g_nasa = 6.67259e-11 | (units.m**3 / units.kg / units.s**2)
  #ms = mg_nasa / g_nasa
  
  sun = Particle()
  sun.name = 'Sun'
  #sun.mass = ms
  sun.mass = 1.0 | units.MSun
  sun.position = [0.,0.,0.] | units.AU
  sun.velocity = [0.,0.,0.] | units.kms
  
  # get the position and velocity vectors relative to sun 
  # by evolving in Kepler
  for i,ecc_i in enumerate(planets_ecc):
    r, v = get_position(sun.mass,
                        planets[i].mass,
                        planets_ecc[i],
                        planets_semi[i],
                        planets_mean_anomaly[i],
                        planets_inclination[i],
                        planets_longitude[i],
                        planets_argument[i],
                        delta_t=delta_JD)
    planets[i].position = r
    planets[i].velocity = v
    
  return sun, planets
コード例 #36
0
def evolve_triple_with_wind(M1, M2, M3, Pora, Pin_0, ain_0, aout_0,
                            ein_0, eout_0, t_end, nsteps, scheme, integrator,
                            t_stellar, dt_se, dtse_fac, interp):

    import random
    from amuse.ext.solarsystem import get_position

    numpy.random.seed(42)

    print("Initial masses:", M1, M2, M3)
    triple = Particles(3)
    triple[0].mass = M1
    triple[1].mass = M2
    triple[2].mass = M3
    stellar = SeBa()
    stellar.particles.add_particles(triple)
    channel_from_stellar = stellar.particles.new_channel_to(triple)

    # Evolve to t_stellar.
    
    stellar.evolve_model(t_stellar)
    channel_from_stellar.copy_attributes(["mass"])
    M1 = triple[0].mass
    M2 = triple[1].mass
    M3 = triple[2].mass
    print("t=", stellar.model_time.in_(units.Myr))
    print("M=", stellar.particles.mass.in_(units.MSun))
    print("R=", stellar.particles.radius.in_(units.RSun))
    print("L=", stellar.particles.luminosity.in_(units.LSun))
    print("T=", stellar.particles.temperature.in_(units.K))
    print("Mdot=", \
        -stellar.particles.wind_mass_loss_rate.in_(units.MSun/units.yr))

    # Start the dynamics.
    # Inner binary:
    
    tmp_stars = Particles(2)
    tmp_stars[0].mass = M1
    tmp_stars[1].mass = M2

    if Pora == 1:
        ain_0 = semimajor_axis(Pin_0, M1+M2)
    else:
        Pin_0 = orbital_period(ain_0, M1+M2)
    print('Pin =', Pin_0)
        
    print('ain_0 =', ain_0)
    print('M1+M2 =', M1+M2)
    print('Pin_0 =', Pin_0.value_in(units.day), '[day]')
    #print 'semi:', semimajor_axis(Pin_0, M1+M2).value_in(units.AU), 'AU'
    #print 'period:', orbital_period(ain_0, M1+M2).value_in(units.day), '[day]'
    
    dt_init = 0.01*Pin_0
    ma = 180
    inc = 60
    aop = 180
    lon = 0
    r,v = get_position(M1, M2, ein_0, ain_0, ma, inc, aop, lon, dt_init)
    tmp_stars[1].position = r
    tmp_stars[1].velocity = v
    tmp_stars.move_to_center()

    # Outer binary:
    
    r,v = get_position(M1+M2, M3, eout_0, aout_0, 0, 0, 0, 0, dt_init)
    tertiary = Particle()
    tertiary.mass = M3
    tertiary.position = r
    tertiary.velocity = v
    tmp_stars.add_particle(tertiary)
    tmp_stars.move_to_center()

    triple.position = tmp_stars.position
    triple.velocity = tmp_stars.velocity

    Mtriple = triple.mass.sum()
    Pout = orbital_period(aout_0, Mtriple)

    print("T=", stellar.model_time.in_(units.Myr))
    print("M=", stellar.particles.mass.in_(units.MSun))
    print("Pout=", Pout.in_(units.Myr))
    print('tK =', ((M1+M2)/M3)*Pout**2*(1-eout_0**2)**1.5/Pin_0)

    converter = nbody_system.nbody_to_si(triple.mass.sum(), aout_0)

    if integrator == 0:
        gravity = Hermite(converter)
        gravity.parameters.timestep_parameter = 0.01
    elif integrator == 1:
        gravity = SmallN(converter)
        gravity.parameters.timestep_parameter = 0.01
        gravity.parameters.full_unperturbed = 0
    elif integrator == 2:
        gravity = Huayno(converter)
        gravity.parameters.inttype_parameter = 20
        gravity.parameters.timestep = (1./256)*Pin_0
    else:
        gravity = symple(converter)
        gravity.parameters.integrator = 10
        #gravity.parameters.timestep_parameter = 0.
        gravity.parameters.timestep = (1./128)*Pin_0

    print(gravity.parameters)

    gravity.particles.add_particles(triple)
    channel_from_framework_to_gd = triple.new_channel_to(gravity.particles)
    channel_from_gd_to_framework = gravity.particles.new_channel_to(triple)
    
    Etot_init = gravity.kinetic_energy + gravity.potential_energy
    Etot_prev = Etot_init

    gravity.particles.move_to_center()

    # Note: time = t_diag = 0 at the start of the dynamical integration.
    
    dt_diag = t_end/float(nsteps)
    t_diag = dt_diag
    time = 0.0 | t_end.unit
    t_se = t_stellar + time

    print('t_end =', t_end)
    print('dt_diag =', dt_diag)

    ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
    print("Triple elements t=",  time,  \
        "inner:", triple[0].mass, triple[1].mass, ain, ein, \
        "outer:", triple[2].mass, aout, eout)

    t = [time.value_in(units.Myr)]
    Mtot = triple.mass.sum()
    mtot = [Mtot.value_in(units.MSun)]
    smai = [ain/ain_0] 
    ecci = [ein/ein_0]
    smao = [aout/aout_0] 
    ecco = [eout/eout_0]

    if interp:
        
        # Create arrays of stellar times and masses for interpolation.

        times = [time]
        masses = [triple.mass.copy()]
        while time < t_end:
            time += dt_se
            stellar.evolve_model(t_stellar+time)
            channel_from_stellar.copy_attributes(["mass"])
            times.append(time)
            masses.append(triple.mass.copy())

        time = 0.0 | t_end.unit
        print('\ntimes:', times, '\n')

    # Evolve the system.
    
    def advance_stellar(t_se, dt):
        E0 = gravity.kinetic_energy + gravity.potential_energy
        t_se += dt

        if interp:
            t = t_se-t_stellar
            i = int(t/dt_se)
            mass = masses[i] + (t-times[i])*(masses[i+1]-masses[i])/dt_se
            triple.mass = mass
            #print 't_se =', t_se, 'masses =', mass
        else:
            stellar.evolve_model(t_se)
            channel_from_stellar.copy_attributes(["mass"])

        channel_from_framework_to_gd.copy_attributes(["mass"])
        return t_se, gravity.kinetic_energy + gravity.potential_energy - E0

    def advance_gravity(tg, dt):
        tg += dt
        gravity.evolve_model(tg)
        channel_from_gd_to_framework.copy()
        return tg

    while time < t_end:

        if scheme == 1:

            # Advance to the next diagnostic time.
            
            dE_se = zero
            dt = t_diag - time

            if dt > 0|dt.unit:
                time = advance_gravity(time, dt)

        elif scheme == 2:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                t_se, dE_se = advance_stellar(t_se, dt)
                time = advance_gravity(time, dt)
            
        elif scheme == 3:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                time = advance_gravity(time, dt)
                t_se, dE_se = advance_stellar(t_se, dt)
            
        elif scheme == 4:
            
            # Derive dt from Pin using dtse_fac.
            
            dt = dtse_fac*Pin_0
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:
                t_se, dE_se = advance_stellar(t_se, 0.5*dt)
                time = advance_gravity(time, dt)
                t_se, dE_se2 = advance_stellar(t_se, 0.5*dt)
                dE_se += dE_se2
            
        elif scheme == 5:

            # Use the specified dt_se.
            
            dE_se = zero
            dt = dt_se
            if time + dt > t_diag: dt = t_diag - time

            if dt > 0|dt.unit:

                # For use with symple only: set up average mass loss.
    
                channel_from_stellar.copy_attributes(["mass"])
                m0 = triple.mass.copy()
                stellar.evolve_model(t_se+dt)
                channel_from_stellar.copy_attributes(["mass"])
                t_se = stellar.model_time
                m1 = triple.mass
                dmdt = (m1-m0)/dt
                for i in range(len(dmdt)):
                    gravity.set_dmdt(i, dmdt[i])

                time = advance_gravity(time, dt)

        else:

            print('unknown option')
            sys.exit(0)

        if time >= t_diag:
            
            t_diag = time + dt_diag

            Ekin = gravity.kinetic_energy 
            Epot = gravity.potential_energy
            Etot = Ekin + Epot
            dE = Etot_prev - Etot
            Mtot = triple.mass.sum()
            print("T=", time, end=' ') 
            print("M=", Mtot, "(dM[SE]=", Mtot/Mtriple, ")", end=' ')
            print("E= ", Etot, "Q= ", Ekin/Epot, end=' ')
            print("dE=", (Etot_init-Etot)/Etot, "ddE=", (Etot_prev-Etot)/Etot, end=' ') 
            print("(dE[SE]=", dE_se/Etot, ")")
            Etot_init -= dE
            Etot_prev = Etot
            ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
            print("Triple elements t=",  t_stellar + time,  \
                "inner:", triple[0].mass, triple[1].mass, ain, ein, \
                "outer:", triple[2].mass, aout, eout)

            t.append(time.value_in(units.yr))
            mtot.append(Mtot.value_in(units.MSun))
            smai.append(ain/ain_0)
            ecci.append(ein/ein_0)
            smao.append(aout/aout_0)
            ecco.append(eout/eout_0)

            if eout > 1 or aout <= zero:
                print("Binary ionized or merged")
                break

    gravity.stop()
    stellar.stop()

    return t, mtot, smai, ecci, smao, ecco
コード例 #37
0
ファイル: h2region.py プロジェクト: yon23/amuse-framework
def main(number_of_grid_cells=15, min_convergence=20):
    inner_radius = 30.0e17 | units.cm
    outer_radius = 95.0e17 | units.cm

    hydrogen_density = 100 | units.cm**-3

    star = Particle()
    star.position = [0.0, 0.0, 0.0] | units.AU
    star.temperature = 20000 | units.K
    star.luminosity = 600.5 | 1e37 * units.erg * (units.s**-1)

    grid = make_grid(number_of_grid_cells=number_of_grid_cells,
                     length=outer_radius,
                     constant_hydrogen_density=hydrogen_density,
                     inner_radius=inner_radius,
                     outer_radius=outer_radius)

    radiative_transfer = Mocassin(number_of_workers=2)  # , debugger = "xterm")

    radiative_transfer.set_input_directory(
        radiative_transfer.get_default_input_directory())
    radiative_transfer.set_mocassin_output_directory(
        radiative_transfer.output_directory + os.sep)

    radiative_transfer.initialize_code()

    radiative_transfer.set_symmetricXYZ(True)

    radiative_transfer.parameters.length_x = outer_radius
    radiative_transfer.parameters.length_y = outer_radius
    radiative_transfer.parameters.length_z = outer_radius
    radiative_transfer.parameters.mesh_size = [
        number_of_grid_cells, number_of_grid_cells, number_of_grid_cells
    ]
    setup_abundancies(radiative_transfer)

    radiative_transfer.parameters.initial_nebular_temperature = 6000.0 | units.K
    radiative_transfer.parameters.high_limit_of_the_frequency_mesh = 15 | mocassin_rydberg_unit
    radiative_transfer.parameters.low_limit_of_the_frequency_mesh = 1.001e-5 | mocassin_rydberg_unit

    radiative_transfer.parameters.total_number_of_photons = 10000000
    radiative_transfer.parameters.total_number_of_points_in_frequency_mesh = 600
    radiative_transfer.parameters.convergence_limit = 0.09
    radiative_transfer.parameters.number_of_ionisation_stages = 6

    radiative_transfer.commit_parameters()
    radiative_transfer.grid.hydrogen_density = grid.hydrogen_density
    radiative_transfer.commit_grid()
    radiative_transfer.particles.add_particle(star)
    radiative_transfer.commit_particles()

    max_number_of_photons = radiative_transfer.parameters.total_number_of_photons * 100

    previous_percentage_converged = 0.0

    for i in range(20):
        radiative_transfer.step()

        percentage_converged = radiative_transfer.get_percentage_converged()
        print("percentage converged :", percentage_converged, ", step :", i,
              ", photons:",
              radiative_transfer.parameters.total_number_of_photons)

        if percentage_converged >= min_convergence:
            break

        if previous_percentage_converged > 5 and percentage_converged < 95:
            convergence_increase = (
                percentage_converged -
                previous_percentage_converged) / previous_percentage_converged
            if (convergence_increase < 0.2
                    and radiative_transfer.parameters.total_number_of_photons <
                    max_number_of_photons):
                radiative_transfer.parameters.total_number_of_photons *= 2

        previous_percentage_converged = percentage_converged

    grid.electron_temperature = radiative_transfer.grid.electron_temperature

    radius = grid.radius.flatten()
    electron_temperature = grid.electron_temperature.flatten()
    selection = electron_temperature > 0 | units.K

    plot_temperature_line(radius[selection], electron_temperature[selection])

    write_set_to_file(grid, 'h2region.h5', 'amuse')
コード例 #38
0
def evolve_triple_with_wind(M1, M2, M3, Pora, Pin_0, ain_0, aout_0,
                            ein_0, eout_0, t_end, nsteps, scheme, dtse_fac):

    import random
    from amuse.ext.solarsystem import get_position

    print "Initial masses:", M1, M2, M3
    t_stellar = 4.0|units.Myr
    triple = Particles(3)
    triple[0].mass = M1
    triple[1].mass = M2
    triple[2].mass = M3
    stellar = SeBa()
    stellar.particles.add_particles(triple)
    channel_from_stellar = stellar.particles.new_channel_to(triple)
    stellar.evolve_model(t_stellar)
    channel_from_stellar.copy_attributes(["mass"])
    M1 = triple[0].mass
    M2 = triple[1].mass
    M3 = triple[2].mass
    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Masses at time T:", M1, M2, M3
    
    # Inner binary
    
    tmp_stars = Particles(2)
    tmp_stars[0].mass = M1
    tmp_stars[1].mass = M2

    if Pora == 1:
        ain_0 = semimajor_axis(Pin_0, M1+M2)
    else:
        Pin_0 = orbital_period(ain_0, M1+M2)
        
    print 'ain_0 =', ain_0
    print 'M1+M2 =', M1+M2
    print 'Pin_0 =', Pin_0.value_in(units.day), '[day]'
    #print 'semi:', semimajor_axis(Pin_0, M1+M2).value_in(units.AU), 'AU'
    #print 'period:', orbital_period(ain_0, M1+M2).value_in(units.day), '[day]'
    
    dt = 0.1*Pin_0
    ma = 180
    inc = 30
    aop = 180
    lon = 0
    r, v = get_position(M1, M2, ein_0, ain_0, ma, inc, aop, lon, dt)
    tmp_stars[1].position = r
    tmp_stars[1].velocity = v
    tmp_stars.move_to_center()

    # Outer binary
    
    r, v = get_position(M1+M2, M3, eout_0, aout_0, 0, 0, 0, 0, dt)
    tertiary = Particle()
    tertiary.mass = M3
    tertiary.position = r
    tertiary.velocity = v
    tmp_stars.add_particle(tertiary)
    tmp_stars.move_to_center()

    triple.position = tmp_stars.position
    triple.velocity = tmp_stars.velocity

    Mtriple = triple.mass.sum()
    Pout = orbital_period(aout_0, Mtriple)

    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Pout=", Pout.in_(units.Myr)

    converter = nbody_system.nbody_to_si(triple.mass.sum(), aout_0)
    gravity = Hermite(converter)
    gravity.particles.add_particles(triple)

    channel_from_framework_to_gd = triple.new_channel_to(gravity.particles)
    channel_from_gd_to_framework = gravity.particles.new_channel_to(triple)
    
    Etot_init = gravity.kinetic_energy + gravity.potential_energy
    Etot_prev = Etot_init

    gravity.particles.move_to_center()

    time = 0.0 | t_end.unit
    ts = t_stellar + time

    ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
    print "Triple elements t=",  time,  \
        "inner:", triple[0].mass, triple[1].mass, ain, ein, \
        "outer:", triple[2].mass, aout, eout

    dt_diag = t_end/float(nsteps)
    t_diag = dt_diag

    t = [time.value_in(units.Myr)] 
    smai = [ain/ain_0] 
    ecci = [ein/ein_0]
    smao = [aout/aout_0] 
    ecco = [eout/eout_0]
    ain = ain_0

    def advance_stellar(ts, dt):
        E0 = gravity.kinetic_energy + gravity.potential_energy
        ts += dt
        stellar.evolve_model(ts)
        channel_from_stellar.copy_attributes(["mass"])
        channel_from_framework_to_gd.copy_attributes(["mass"])
        return ts, gravity.kinetic_energy + gravity.potential_energy - E0

    def advance_gravity(tg, dt):
        tg += dt
        gravity.evolve_model(tg)
        channel_from_gd_to_framework.copy()
        return tg

    while time < t_end:

        Pin = orbital_period(ain, triple[0].mass+triple[1].mass)
        dt = dtse_fac*Pin
        dt *= random.random()

        if scheme == 1:
            
            ts, dE_se = advance_stellar(ts, dt)
            time = advance_gravity(time, dt)
            
        elif scheme == 2:
            
            time = advance_gravity(time, dt)
            ts, dE_se = advance_stellar(ts, dt)
            
        else:

            dE_se = zero
            #ts, dE_se = advance_stellar(ts, dt/2)
            time = advance_gravity(time, dt)
            #ts, dE = advance_stellar(ts, dt/2)
            #dE_se += dE

        if time >= t_diag:
            
            t_diag = time + dt_diag

            Ekin = gravity.kinetic_energy 
            Epot = gravity.potential_energy
            Etot = Ekin + Epot
            dE = Etot_prev - Etot
            Mtot = triple.mass.sum()
            print "T=", time, 
            print "M=", Mtot, "(dM[SE]=", Mtot/Mtriple, ")",
            print "E= ", Etot, "Q= ", Ekin/Epot,
            print "dE=", (Etot_init-Etot)/Etot, "ddE=", (Etot_prev-Etot)/Etot, 
            print "(dE[SE]=", dE_se/Etot, ")"
            Etot_init -= dE
            Etot_prev = Etot
            ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
            print "Triple elements t=",  (4|units.Myr) + time,  \
                "inner:", triple[0].mass, triple[1].mass, ain, ein, \
                "outer:", triple[2].mass, aout, eout

            t.append(time.value_in(units.Myr))
            smai.append(ain/ain_0)
            ecci.append(ein/ein_0)
            smao.append(aout/aout_0)
            ecco.append(eout/eout_0)

            if eout > 1.0 or aout <= zero:
                print "Binary ionized or merged"
                break

    gravity.stop()
    stellar.stop()

    return t, smai, ecci, smao, ecco
コード例 #39
0
def evolve_triple_with_wind(M1, M2, M3, Pora, Pin_0, ain_0, aout_0,
                            ein_0, eout_0, t_end, nsteps, scheme, dtse_fac):

    import random
    from amuse.ext.solarsystem import get_position

    print "Initial masses:", M1, M2, M3
    t_stellar = 4.0|units.Myr
    triple = Particles(3)
    triple[0].mass = M1
    triple[1].mass = M2
    triple[2].mass = M3
    stellar = SeBa()
    stellar.particles.add_particles(triple)
    channel_from_stellar = stellar.particles.new_channel_to(triple)
    stellar.evolve_model(t_stellar)
    channel_from_stellar.copy_attributes(["mass"])
    M1 = triple[0].mass
    M2 = triple[1].mass
    M3 = triple[2].mass
    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Masses at time T:", M1, M2, M3
    
    # Inner binary
    
    tmp_stars = Particles(2)
    tmp_stars[0].mass = M1
    tmp_stars[1].mass = M2

    if Pora == 1:
        ain_0 = semimajor_axis(Pin_0, M1+M2)
    else:
        Pin_0 = orbital_period(ain_0, M1+M2)
        
    print 'ain_0 =', ain_0
    print 'M1+M2 =', M1+M2
    print 'Pin_0 =', Pin_0.value_in(units.day), '[day]'
    #print 'semi:', semimajor_axis(Pin_0, M1+M2).value_in(units.AU), 'AU'
    #print 'period:', orbital_period(ain_0, M1+M2).value_in(units.day), '[day]'
    
    dt = 0.1*Pin_0
    ma = 180
    inc = 30
    aop = 180
    lon = 0
    r, v = get_position(M1, M2, ein_0, ain_0, ma, inc, aop, lon, dt)
    tmp_stars[1].position = r
    tmp_stars[1].velocity = v
    tmp_stars.move_to_center()

    # Outer binary
    
    r, v = get_position(M1+M2, M3, eout_0, aout_0, 0, 0, 0, 0, dt)
    tertiary = Particle()
    tertiary.mass = M3
    tertiary.position = r
    tertiary.velocity = v
    tmp_stars.add_particle(tertiary)
    tmp_stars.move_to_center()

    triple.position = tmp_stars.position
    triple.velocity = tmp_stars.velocity

    Mtriple = triple.mass.sum()
    Pout = orbital_period(aout_0, Mtriple)

    print "T=", stellar.model_time.in_(units.Myr)
    print "M=", stellar.particles.mass.in_(units.MSun)
    print "Pout=", Pout.in_(units.Myr)

    converter = nbody_system.nbody_to_si(triple.mass.sum(), aout_0)
    gravity = Hermite(converter)
    gravity.particles.add_particles(triple)

    channel_from_framework_to_gd = triple.new_channel_to(gravity.particles)
    channel_from_gd_to_framework = gravity.particles.new_channel_to(triple)
    
    Etot_init = gravity.kinetic_energy + gravity.potential_energy
    Etot_prev = Etot_init

    gravity.particles.move_to_center()

    time = 0.0 | t_end.unit
    ts = t_stellar + time

    ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
    print "Triple elements t=",  time,  \
        "inner:", triple[0].mass, triple[1].mass, ain, ein, \
        "outer:", triple[2].mass, aout, eout

    dt_diag = t_end/float(nsteps)
    t_diag = dt_diag

    t = [time.value_in(units.Myr)] 
    smai = [ain/ain_0] 
    ecci = [ein/ein_0]
    smao = [aout/aout_0] 
    ecco = [eout/eout_0]
    ain = ain_0

    def advance_stellar(ts, dt):
        E0 = gravity.kinetic_energy + gravity.potential_energy
        ts += dt
        stellar.evolve_model(ts)
        channel_from_stellar.copy_attributes(["mass"])
        channel_from_framework_to_gd.copy_attributes(["mass"])
        return ts, gravity.kinetic_energy + gravity.potential_energy - E0

    def advance_gravity(tg, dt):
        tg += dt
        gravity.evolve_model(tg)
        channel_from_gd_to_framework.copy()
        return tg

    while time < t_end:

        Pin = orbital_period(ain, triple[0].mass+triple[1].mass)
        dt = dtse_fac*Pin
        dt *= random.random()

        if scheme == 1:
            
            ts, dE_se = advance_stellar(ts, dt)
            time = advance_gravity(time, dt)
            
        elif scheme == 2:
            
            time = advance_gravity(time, dt)
            ts, dE_se = advance_stellar(ts, dt)
            
        else:

            dE_se = zero
            #ts, dE_se = advance_stellar(ts, dt/2)
            time = advance_gravity(time, dt)
            #ts, dE = advance_stellar(ts, dt/2)
            #dE_se += dE

        if time >= t_diag:
            
            t_diag = time + dt_diag

            Ekin = gravity.kinetic_energy 
            Epot = gravity.potential_energy
            Etot = Ekin + Epot
            dE = Etot_prev - Etot
            Mtot = triple.mass.sum()
            print "T=", time, 
            print "M=", Mtot, "(dM[SE]=", Mtot/Mtriple, ")",
            print "E= ", Etot, "Q= ", Ekin/Epot,
            print "dE=", (Etot_init-Etot)/Etot, "ddE=", (Etot_prev-Etot)/Etot, 
            print "(dE[SE]=", dE_se/Etot, ")"
            Etot_init -= dE
            Etot_prev = Etot
            ain, ein, aout, eout = get_orbital_elements_of_triple(triple)
            print "Triple elements t=",  (4|units.Myr) + time,  \
                "inner:", triple[0].mass, triple[1].mass, ain, ein, \
                "outer:", triple[2].mass, aout, eout

            t.append(time.value_in(units.Myr))
            smai.append(ain/ain_0)
            ecci.append(ein/ein_0)
            smao.append(aout/aout_0)
            ecco.append(eout/eout_0)

            if eout > 1.0 or aout <= zero:
                print "Binary ionized or merged"
                break

    gravity.stop()
    stellar.stop()

    return t, smai, ecci, smao, ecco
コード例 #40
0
ファイル: h2region.py プロジェクト: amusecode/amuse
def main(number_of_grid_cells=15, min_convergence=20):
    inner_radius = 30.0e17 | units.cm
    outer_radius = 95.0e17 | units.cm

    hydrogen_density = 100 | units.cm ** -3

    star = Particle()
    star.position = [0.0, 0.0, 0.0] | units.AU
    star.temperature = 20000 | units.K
    star.luminosity = 600.5 | 1e37 * units.erg * (units.s**-1)

    grid = make_grid(
        number_of_grid_cells=number_of_grid_cells,
        length=outer_radius,
        constant_hydrogen_density=hydrogen_density,
        inner_radius=inner_radius,
        outer_radius=outer_radius
    )

    radiative_transfer = Mocassin(number_of_workers=2)  # , debugger = "xterm")

    radiative_transfer.set_input_directory(
        radiative_transfer.get_default_input_directory())
    radiative_transfer.set_mocassin_output_directory(
        radiative_transfer.output_directory + os.sep)

    radiative_transfer.initialize_code()

    radiative_transfer.set_symmetricXYZ(True)

    radiative_transfer.parameters.length_x = outer_radius
    radiative_transfer.parameters.length_y = outer_radius
    radiative_transfer.parameters.length_z = outer_radius
    radiative_transfer.parameters.mesh_size = [
        number_of_grid_cells, number_of_grid_cells, number_of_grid_cells]
    setup_abundancies(radiative_transfer)

    radiative_transfer.parameters.initial_nebular_temperature = 6000.0 | units.K
    radiative_transfer.parameters.high_limit_of_the_frequency_mesh = 15 | mocassin_rydberg_unit
    radiative_transfer.parameters.low_limit_of_the_frequency_mesh = 1.001e-5 | mocassin_rydberg_unit

    radiative_transfer.parameters.total_number_of_photons = 10000000
    radiative_transfer.parameters.total_number_of_points_in_frequency_mesh = 600
    radiative_transfer.parameters.convergence_limit = 0.09
    radiative_transfer.parameters.number_of_ionisation_stages = 6

    radiative_transfer.commit_parameters()
    radiative_transfer.grid.hydrogen_density = grid.hydrogen_density
    radiative_transfer.commit_grid()
    radiative_transfer.particles.add_particle(star)
    radiative_transfer.commit_particles()

    max_number_of_photons = radiative_transfer.parameters.total_number_of_photons * 100

    previous_percentage_converged = 0.0

    for i in range(20):
        radiative_transfer.step()

        percentage_converged = radiative_transfer.get_percentage_converged()
        print(
                "percentage converged :", percentage_converged,
                ", step :", i,
                ", photons:",
                radiative_transfer.parameters.total_number_of_photons)

        if percentage_converged >= min_convergence:
            break

        if previous_percentage_converged > 5 and percentage_converged < 95:
            convergence_increase = (
                percentage_converged - previous_percentage_converged
                ) / previous_percentage_converged
            if (
                    convergence_increase < 0.2
                    and radiative_transfer.parameters.total_number_of_photons < max_number_of_photons
                    ):
                radiative_transfer.parameters.total_number_of_photons *= 2

        previous_percentage_converged = percentage_converged

    grid.electron_temperature = radiative_transfer.grid.electron_temperature

    radius = grid.radius.flatten()
    electron_temperature = grid.electron_temperature.flatten()
    selection = electron_temperature > 0 | units.K

    plot_temperature_line(radius[selection], electron_temperature[selection])

    write_set_to_file(grid, 'h2region.h5', 'amuse')