diff options
| -rw-r--r-- | Docs/source/usage/parameters.rst | 8 | ||||
| -rw-r--r-- | Regression/Checksum/benchmarks_json/hard_edged_plasma_lens.json (renamed from Regression/Checksum/benchmarks_json/hard_edged_lasma_lens.json) | 0 | ||||
| -rw-r--r-- | Regression/WarpX-tests.ini | 2 |
3 files changed, 5 insertions, 5 deletions
diff --git a/Docs/source/usage/parameters.rst b/Docs/source/usage/parameters.rst index 3a258a295..d518b7866 100644 --- a/Docs/source/usage/parameters.rst +++ b/Docs/source/usage/parameters.rst @@ -1323,7 +1323,7 @@ Grid initialization then the constants `Bo` and `delta` required in the above equation can be set using ``my_constants.Bo=`` and ``my_constants.delta=`` in the input file. For a two-dimensional simulation, it is assumed that the first dimension - is `x` and the second dimension in `z`, and the value of `y` is set to zero. + is `x` and the second dimension is `z`, and the value of `y` is set to zero. Note that the current implementation of the parser for external B-field does not work with RZ and the code will abort with an error message. @@ -1347,7 +1347,7 @@ Grid initialization then the constants `Bo` and `delta` required in the above equation can be set using ``my_constants.Eo=`` and ``my_constants.delta=`` in the input file. For a two-dimensional simulation, it is assumed that the first - dimension is `x` and the second dimension in `z`, + dimension is `x` and the second dimension is `z`, and the value of `y` is set to zero. Note that the current implementation of the parser for external E-field does not work with RZ and the code will abort with an error message. @@ -1644,12 +1644,12 @@ Numerics and algorithms The ratio between the actual timestep that is used in the simulation and the Courant-Friedrichs-Lewy (CFL) limit. (e.g. for `warpx.cfl=1`, the timestep will be exactly equal to the CFL limit.) - This parameter will only be used with the electromagnatic solver. + This parameter will only be used with the electromagnetic solver. * ``warpx.const_dt`` (`float`) Allows direct specification of the time step size, in units of seconds. When the electrostatic solver is being used, this must be supplied. - This can be used with the electromagnatic solver, overriding ``warpx.cfl``, but + This can be used with the electromagnetic solver, overriding ``warpx.cfl``, but it is up to the user to ensure that the CFL condition is met. * ``warpx.use_filter`` (`0` or `1`; default: `1`, except for RZ FDTD) diff --git a/Regression/Checksum/benchmarks_json/hard_edged_lasma_lens.json b/Regression/Checksum/benchmarks_json/hard_edged_plasma_lens.json index 34d356987..34d356987 100644 --- a/Regression/Checksum/benchmarks_json/hard_edged_lasma_lens.json +++ b/Regression/Checksum/benchmarks_json/hard_edged_plasma_lens.json diff --git a/Regression/WarpX-tests.ini b/Regression/WarpX-tests.ini index 954cfe22a..d892b687b 100644 --- a/Regression/WarpX-tests.ini +++ b/Regression/WarpX-tests.ini @@ -3349,7 +3349,7 @@ compareParticles = 1 particleTypes = electron analysisRoutine = Examples/Tests/AcceleratorLattice/analysis.py -[hard_edged_lasma_lens] +[hard_edged_plasma_lens] buildDir = . inputFile = Examples/Tests/plasma_lens/inputs_lattice_3d runtime_params = |