You signed in with another tab or window. Reload to refresh your session.You signed out in another tab or window. Reload to refresh your session.You switched accounts on another tab or window. Reload to refresh your session.Dismiss alert
``t`` represents the physical time in seconds during the simulation.
1471
+
``x``, ``y``, ``z`` represent particle positions in the unit of meter.
1472
+
``ux``, ``uy``, ``uz`` represent the particle momenta in the unit of
1473
+
:math:`\gamma v/c`, where
1474
+
:math:`\gamma` is the Lorentz factor,
1475
+
:math:`v/c` is the particle velocity normalized by the speed of light.
1475
1476
1476
1477
* ``<species_name>.save_particles_at_xlo/ylo/zlo``, ``<species_name>.save_particles_at_xhi/yhi/zhi`` and ``<species_name>.save_particles_at_eb`` (`0` or `1` optional, default `0`)
1477
1478
If `1` particles of this species will be copied to the scraped particle
@@ -2546,7 +2547,7 @@ Particle push, charge and current deposition, field gathering
2546
2547
- ``vay``: Vay pusher (see :cite:t:`param-Vaypop2008`)
2547
2548
- ``higuera``: Higuera-Cary pusher (see :cite:t:`param-HigueraPOP2017`)
2548
2549
2549
-
If ``algo.particle_pusher`` is not specified, ``boris`` is the default.
2550
+
If ``algo.particle_pusher`` is not specified, ``boris`` is the default.
2550
2551
2551
2552
* ``algo.particle_shape`` (`integer`; `1`, `2`, `3`, or `4`)
2552
2553
The order of the shape factors (splines) for the macro-particles along all spatial directions: `1` for linear, `2` for quadratic, `3` for cubic, `4` for quartic.
@@ -2576,7 +2577,7 @@ Two families of Maxwell solvers are implemented in WarpX, based on the Finite-Di
2576
2577
- ``hybrid``: The E-field will be solved using Ohm's law and a kinetic-fluid hybrid model (see :ref:`theory <theory-kinetic-fluid-hybrid-model>`).
2577
2578
- ``none``: No field solve will be performed.
2578
2579
2579
-
If ``algo.maxwell_solver`` is not specified, ``yee`` is the default.
2580
+
If ``algo.maxwell_solver`` is not specified, ``yee`` is the default.
2580
2581
2581
2582
* ``algo.em_solver_medium`` (`string`, optional)
2582
2583
The medium for evaluating the Maxwell solver. Available options are :
@@ -2738,10 +2739,10 @@ Maxwell solver: macroscopic media
2738
2739
Comparing the two methods, Lax-Wendroff is more prone to developing oscillations and requires a smaller timestep for stability. On the other hand, Backward Euler is more robust but it is first-order accurate in time compared to the second-order Lax-Wendroff method.
File based: one file per timestep (slower), group/variable based: one file for all steps (faster)).
3072
-
``variable based`` is an `experimental feature with ADIOS2 BP5 <https://openpmd-api.readthedocs.io/en/0.17.0/backends/adios2.html#experimental-new-adios2-schema>`__ that will replace ``g``.
File based: one file per timestep (slower), group/variable based: one file for all steps (faster)).
3073
+
``variable based`` is an `experimental feature with ADIOS2 BP5 <https://openpmd-api.readthedocs.io/en/0.17.0/backends/adios2.html#experimental-new-adios2-schema>`__ that will replace ``g``.
3074
+
Default: ``f`` (full diagnostics)
3074
3075
3075
3076
* ``<diag_name>.buffer_flush_limit_btd`` (`integer`; defaults to 5) optional, only read if ``<diag_name>.diag_type = BackTransformed``
3076
3077
This parameter is intended for ADIOS backend to group every N buffers (N is the value of this parameter) and then flush to disk.
@@ -3140,20 +3141,20 @@ In-situ capabilities can be used by turning on Sensei or Ascent (provided they a
3140
3141
Whether to save all modes when in RZ. When ``openpmd_backend = openpmd``, this parameter is ignored and all modes are saved.
3141
3142
3142
3143
* ``<diag_name>.particle_fields_to_plot`` (list of `strings`, optional)
3143
-
Names of per-cell diagnostics of particle properties to calculate and output as additional fields.
3144
-
Note that the deposition onto the grid does not respect the particle shape factor, but instead uses nearest-grid point interpolation.
3145
-
Default is none.
3146
-
Parser functions for these field names are specified by ``<diag_name>.particle_fields.<field_name>(x,y,z,ux,uy,uz)``.
3147
-
Also, note that this option is only available for ``<diag_name>.diag_type = Full``
3144
+
Names of per-cell diagnostics of particle properties to calculate and output as additional fields.
3145
+
Note that the deposition onto the grid does not respect the particle shape factor, but instead uses nearest-grid point interpolation.
3146
+
Default is none.
3147
+
Parser functions for these field names are specified by ``<diag_name>.particle_fields.<field_name>(x,y,z,ux,uy,uz)``.
3148
+
Also, note that this option is only available for ``<diag_name>.diag_type = Full``
3148
3149
3149
3150
* ``<diag_name>.particle_fields_species`` (list of `strings`, optional)
3150
-
Species for which to calculate ``particle_fields_to_plot``.
3151
-
Fields will be calculated separately for each specified species.
3152
-
The default is a list of all of the available particle species.
3151
+
Species for which to calculate ``particle_fields_to_plot``.
3152
+
Fields will be calculated separately for each specified species.
3153
+
The default is a list of all of the available particle species.
3153
3154
3154
3155
* ``<diag_name>.particle_fields.<field_name>.do_average`` (`0` or `1`) optional (default `1`)
3155
-
Whether the diagnostic is an average or a sum. With an average, the sum over the specified function is divided
3156
-
by the sum of the particle weights in each cell.
3156
+
Whether the diagnostic is an average or a sum. With an average, the sum over the specified function is divided
0 commit comments