zmin = -20.e-6
rmax = +20.e-6
zmax = +20.e-6
uniform_plasma = picmi.UniformDistribution(density=1.e25,
upper_bound=[None, None, 0.],
directed_velocity=[0., 0., 0.1])
electrons = picmi.Species(particle_type='electron',
name='electrons',
initial_distribution=uniform_plasma)
grid = picmi.CylindricalGrid(
number_of_cells=[nr, nz],
lower_bound=[rmin, zmin],
upper_bound=[rmax, zmax],
lower_boundary_conditions=['dirichlet', 'periodic'],
upper_boundary_conditions=['dirichlet', 'periodic'],
moving_window_velocity=[0., 0.],
warpx_max_grid_size=32)
solver = picmi.ElectromagneticSolver(grid=grid, cfl=1.)
sim = picmi.Simulation(solver=solver,
max_steps=40,
verbose=1,
warpx_plot_int=1,
warpx_current_deposition_algo=3,
warpx_charge_deposition_algo=0,
warpx_field_gathering_algo=0,
warpx_particle_pusher_algo=0)
rmin = 0
rmax = 30e-06
zmin = -56e-06
zmax = 12e-06
# Domain decomposition
max_grid_size = 64
blocking_factor = 32
# Create grid
grid = picmi.CylindricalGrid(
number_of_cells = [nr, nz],
n_azimuthal_modes = 2,
lower_bound = [rmin, zmin],
upper_bound = [rmax, zmax],
lower_boundary_conditions = ['none', 'dirichlet'],
upper_boundary_conditions = ['dirichlet', 'dirichlet'],
lower_boundary_conditions_particles = ['absorbing', 'absorbing'],
upper_boundary_conditions_particles = ['absorbing', 'absorbing'],
moving_window_velocity = [0., c],
warpx_max_grid_size = max_grid_size,
warpx_blocking_factor = blocking_factor)
# Particles: plasma electrons
plasma_density = 2e23
plasma_xmin = -20e-06
plasma_ymin = None
plasma_zmin = 10e-06
plasma_xmax = 20e-06
plasma_ymax = None
plasma_zmax = None
uniform_distribution = picmi.UniformDistribution(
k0=k0,
w0=w0,
momentum_expressions=momentum_expressions)
electrons = picmi.Species(particle_type='electron',
name='electrons',
initial_distribution=analytic_plasma)
protons = picmi.Species(particle_type='proton',
name='protons',
initial_distribution=uniform_plasma)
grid = picmi.CylindricalGrid(
number_of_cells=[nr, nz],
n_azimuthal_modes=3,
lower_bound=[rmin, zmin],
upper_bound=[rmax, zmax],
lower_boundary_conditions=['dirichlet', 'periodic'],
upper_boundary_conditions=['dirichlet', 'periodic'],
moving_window_zvelocity=0.,
warpx_max_grid_size=64)
solver = picmi.ElectromagneticSolver(grid=grid, cfl=1.)
sim = picmi.Simulation(solver=solver,
max_steps=40,
verbose=1,
warpx_plot_int=40,
warpx_current_deposition_algo='esirkepov',
warpx_field_gathering_algo='energy-conserving',
warpx_particle_pusher_algo='boris')
name='electrons',
initial_distribution=analytic_plasma)
protons = picmi.Species(particle_type='proton',
name='protons',
initial_distribution=uniform_plasma)
##########################
# numerics components
##########################
grid = picmi.CylindricalGrid(
number_of_cells=[nr, nz],
n_azimuthal_modes=3,
lower_bound=[rmin, zmin],
upper_bound=[rmax, zmax],
lower_boundary_conditions=['none', 'periodic'],
upper_boundary_conditions=['none', 'periodic'],
lower_boundary_conditions_particles=['absorbing', 'periodic'],
upper_boundary_conditions_particles=['absorbing', 'periodic'],
moving_window_velocity=[0., 0.],
warpx_max_grid_size=64)
solver = picmi.ElectromagneticSolver(grid=grid, cfl=1.)
##########################
# diagnostics
##########################
field_diag1 = picmi.FieldDiagnostic(
name='diag1',
grid=grid,
