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| author |  Dave Grote <grote1@llnl.gov>
| 2019-03-18 16:36:21 -0700 |
|---|---|---|
| committer | Dave Grote <grote1@llnl.gov>
| 2019-03-18 16:36:21 -0700 |
| commit | d0716557190dd1bbc39c835eea18f8c67e22b3cc (patch) | |
| tree | b75f9034d95d3fb60369ffd23c7bdc3346c77579 | |
| parent | 54ff6741b624f1b9162c5d503135f99b895b54d3 (diff) | |
| download | WarpX-d0716557190dd1bbc39c835eea18f8c67e22b3cc.tar.gz WarpX-d0716557190dd1bbc39c835eea18f8c67e22b3cc.tar.zst WarpX-d0716557190dd1bbc39c835eea18f8c67e22b3cc.zip | |
Removed more references to warpx_coord_sys
4 files changed, 4 insertions, 4 deletions
diff --git a/Examples/Modules/gaussian_beam/gaussian_beam_PICMI.py b/Examples/Modules/gaussian_beam/gaussian_beam_PICMI.py index 641855e9a..b9bfc2864 100644 --- a/Examples/Modules/gaussian_beam/gaussian_beam_PICMI.py +++ b/Examples/Modules/gaussian_beam/gaussian_beam_PICMI.py @@ -26,7 +26,7 @@ grid = picmi.Cartesian3DGrid(number_of_cells = [nx, ny, nz], upper_bound = [xmax, ymax, zmax], lower_boundary_conditions = ['periodic', 'periodic', 'open'], upper_boundary_conditions = ['periodic', 'periodic', 'open'], - warpx_max_grid_size=16, warpx_coord_sys=0) + warpx_max_grid_size=16) solver = picmi.ElectromagneticSolver(grid = grid, cfl = 1., diff --git a/Examples/Physics_applications/laser_acceleration/laser_acceleration_PICMI.py b/Examples/Physics_applications/laser_acceleration/laser_acceleration_PICMI.py index 867e7a951..3094a9db5 100644 --- a/Examples/Physics_applications/laser_acceleration/laser_acceleration_PICMI.py +++ b/Examples/Physics_applications/laser_acceleration/laser_acceleration_PICMI.py @@ -89,7 +89,7 @@ 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, - warpx_max_grid_size=32, warpx_coord_sys=0) + warpx_max_grid_size=32) solver = picmi.ElectromagneticSolver(grid=grid, method='CKC', cfl=1.) diff --git a/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.mr.py b/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.mr.py index 3cb3ba1dc..563fe110e 100644 --- a/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.mr.py +++ b/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.mr.py @@ -25,7 +25,7 @@ grid = picmi.Cartesian3DGrid(number_of_cells = [nx, ny, nz], upper_boundary_conditions = ['periodic', 'periodic', 'open'], moving_window_velocity = moving_window_velocity, #refined_regions = [[1, [-25e-6, -25e-6, -200.e-6], [25e-6, 25e-6, 200.e-6]]], # as argument - warpx_max_grid_size=128, warpx_coord_sys=0, warpx_blocking_factor=16) + warpx_max_grid_size=128, warpx_blocking_factor=16) # --- As a seperate function call (instead of refined_regions argument) grid.add_refined_region(level = 1, diff --git a/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.py b/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.py index eddbd558b..0d9a831e3 100644 --- a/Examples/Physics_applications/plasma_acceleration/plasma_acceleration_PICMI.py +++ b/Examples/Physics_applications/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, - warpx_max_grid_size=32, warpx_coord_sys=0) + warpx_max_grid_size=32) solver = picmi.ElectromagneticSolver(grid=grid, cfl=1) |