diff options
Diffstat (limited to 'Example')
| -rw-r--r-- | Example/Langmuir/langmuir_PICMI.py | 10 | ||||
| -rw-r--r-- | Example/laser_acceleration/laser_acceleration_PICMI.py | 10 | ||||
| -rw-r--r-- | Example/plasma_acceleration/plasma_acceleration_PICMI.py | 10 |
3 files changed, 15 insertions, 15 deletions
diff --git a/Example/Langmuir/langmuir_PICMI.py b/Example/Langmuir/langmuir_PICMI.py index 483de8047..0a1200ffa 100644 --- a/Example/Langmuir/langmuir_PICMI.py +++ b/Example/Langmuir/langmuir_PICMI.py @@ -22,7 +22,7 @@ grid = picmi.Cartesian3DGrid(number_of_cells = [nx, ny, nz], lower_boundary_conditions = ['periodic', 'periodic', 'periodic'], upper_boundary_conditions = ['periodic', 'periodic', 'periodic'], moving_window_velocity = [0., 0., 0.], - max_grid_size=32, max_level=0, coord_sys=0) + warpx_max_grid_size=32, warpx_max_level=0, warpx_coord_sys=0) solver = picmi.ElectromagneticSolver(grid=grid, cfl=1.) @@ -30,10 +30,10 @@ sim = picmi.Simulation(solver = solver, verbose = 1, max_steps = 40, plot_int = 1, - current_deposition_algo = 3, - charge_deposition_algo = 0, - field_gathering_algo = 0, - particle_pusher_algo = 0) + warpx_current_deposition_algo = 3, + warpx_charge_deposition_algo = 0, + warpx_field_gathering_algo = 0, + warpx_particle_pusher_algo = 0) sim.add_species(electrons, layout=picmi.GriddedLayout(n_macroparticle_per_cell=[2,2,2], grid=grid)) diff --git a/Example/laser_acceleration/laser_acceleration_PICMI.py b/Example/laser_acceleration/laser_acceleration_PICMI.py index e3fff99bb..4cb906378 100644 --- a/Example/laser_acceleration/laser_acceleration_PICMI.py +++ b/Example/laser_acceleration/laser_acceleration_PICMI.py @@ -26,7 +26,7 @@ grid = picmi.Cartesian3DGrid(number_of_cells = [nx, ny, nz], lower_boundary_conditions = ['periodic', 'periodic', 'open'], upper_boundary_conditions = ['periodic', 'periodic', 'open'], moving_window_velocity = moving_window_velocity, - max_grid_size=32, max_level=0, coord_sys=0) + warpx_max_grid_size=32, warpx_max_level=0, warpx_coord_sys=0) solver = picmi.ElectromagneticSolver(grid=grid, cfl=1.) @@ -59,10 +59,10 @@ sim = picmi.Simulation(solver = solver, verbose = 1, cfl = 1.0, max_steps = 1000, - current_deposition_algo = 3, - charge_deposition_algo = 0, - field_gathering_algo = 0, - particle_pusher_algo = 0) + warpx_current_deposition_algo = 3, + warpx_charge_deposition_algo = 0, + warpx_field_gathering_algo = 0, + warpx_particle_pusher_algo = 0) sim.add_species(electrons, layout=picmi.GriddedLayout(grid=grid, n_macroparticle_per_cell=number_per_cell_each_dim)) diff --git a/Example/plasma_acceleration/plasma_acceleration_PICMI.py b/Example/plasma_acceleration/plasma_acceleration_PICMI.py index 5d16a7928..0d831f3e1 100644 --- a/Example/plasma_acceleration/plasma_acceleration_PICMI.py +++ b/Example/plasma_acceleration/plasma_acceleration_PICMI.py @@ -23,7 +23,7 @@ grid = picmi.Cartesian3DGrid(number_of_cells = [nx, ny, nz], lower_boundary_conditions = ['periodic', 'periodic', 'open'], upper_boundary_conditions = ['periodic', 'periodic', 'open'], moving_window_velocity = moving_window_velocity, - max_grid_size=32, max_level=0, coord_sys=0) + warpx_max_grid_size=32, warpx_max_level=0, warpx_coord_sys=0) solver = picmi.ElectromagneticSolver(grid=grid, cfl=1) @@ -45,10 +45,10 @@ sim = picmi.Simulation(solver = solver, verbose = 1, cfl = 1.0, max_steps = 1000, - current_deposition_algo = 3, - charge_deposition_algo = 0, - field_gathering_algo = 0, - particle_pusher_algo = 0) + warpx_current_deposition_algo = 3, + warpx_charge_deposition_algo = 0, + warpx_field_gathering_algo = 0, + warpx_particle_pusher_algo = 0) sim.add_species(beam, layout=picmi.GriddedLayout(grid=grid, n_macroparticle_per_cell=number_per_cell_each_dim)) sim.add_species(plasma, layout=picmi.GriddedLayout(grid=grid, n_macroparticle_per_cell=number_per_cell_each_dim)) |