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author | 2018-07-30 15:43:03 -0700 | |
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committer | 2018-07-30 15:43:03 -0700 | |
commit | fc784aef722c45fc4e0849b27e24b5583181e00f (patch) | |
tree | 968c28322c295966d4ebb0fad119944ba797ab19 /Example/plasma_acceleration/plasma_acceleration_PICMI.py | |
parent | b0d78403bc8637e56e3d41edd5f39116180067eb (diff) | |
download | WarpX-fc784aef722c45fc4e0849b27e24b5583181e00f.tar.gz WarpX-fc784aef722c45fc4e0849b27e24b5583181e00f.tar.zst WarpX-fc784aef722c45fc4e0849b27e24b5583181e00f.zip |
Use codename as prefix for code specific arguments.
Diffstat (limited to 'Example/plasma_acceleration/plasma_acceleration_PICMI.py')
-rw-r--r-- | Example/plasma_acceleration/plasma_acceleration_PICMI.py | 10 |
1 files changed, 5 insertions, 5 deletions
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)) |