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BLAST-ImpactX · Feb 21, 2025 · b23c9af · b23c9af
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Showing 19 changed files with 19 additions and 19 deletions.
diff --git a/examples/CMakeLists.txt b/examples/CMakeLists.txt
@@ -106,7 +106,7 @@ function(add_impactx_test name input is_mpi analysis_script plot_script)
                         amrex.throw_exception = 1
                         amrex.signal_handling = 0
                         impactx.always_warn_immediately=1
-                        #impactx.abort_on_warning_threshold=low
+                        impactx.abort_on_warning_threshold=low
                         ${INPUTS_ARGS}
                  WORKING_DIRECTORY ${THIS_WORKING_DIR}
         )

diff --git a/examples/cfchannel/input_cfchannel_10nC_fft.in b/examples/cfchannel/input_cfchannel_10nC_fft.in
@@ -37,7 +37,7 @@ constf1.kt = 1.0
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 algo.poisson_solver = "fft"
 
 amr.n_cell = 48 48 40

diff --git a/examples/cfchannel/input_cfchannel_10nC_mlmg.in b/examples/cfchannel/input_cfchannel_10nC_mlmg.in
@@ -37,7 +37,7 @@ constf1.kt = 1.0
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 amr.n_cell = 48 48 40
 #amr.n_cell = 72 72 64  # optional for increased precision

diff --git a/examples/cfchannel/run_cfchannel_10nC_fft.py b/examples/cfchannel/run_cfchannel_10nC_fft.py
@@ -13,7 +13,7 @@
 # set numerical parameters and IO control
 sim.n_cell = [48, 48, 40]  # [72, 72, 64] for increased precision
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.poisson_solver = "fft"
 sim.prob_relative = [1.1]
 # sim.diagnostics = False  # benchmarking

diff --git a/examples/cfchannel/run_cfchannel_10nC_mlmg.py b/examples/cfchannel/run_cfchannel_10nC_mlmg.py
@@ -13,7 +13,7 @@
 # set numerical parameters and IO control
 sim.n_cell = [48, 48, 40]  # [72, 72, 64] for increased precision
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.prob_relative = [3.0]
 # sim.diagnostics = False  # benchmarking
 sim.slice_step_diagnostics = True

diff --git a/examples/epac2004_benchmarks/input_bithermal.in b/examples/epac2004_benchmarks/input_bithermal.in
@@ -36,7 +36,7 @@ constf1.nslice = 50
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 #amr.n_cell = 128 128 128  #full resolution
 amr.n_cell = 64 64 64

diff --git a/examples/epac2004_benchmarks/input_fodo_rf_SC.in b/examples/epac2004_benchmarks/input_fodo_rf_SC.in
@@ -117,7 +117,7 @@ gapb1.sin_coefficients = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0  \
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 amr.n_cell = 56 56 64
 geometry.prob_relative = 4.0

diff --git a/examples/epac2004_benchmarks/input_thermal.in b/examples/epac2004_benchmarks/input_thermal.in
@@ -33,7 +33,7 @@ constf1.nslice = 400   #full resolution
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 #amr.n_cell = 128 128 128  #full resolution
 amr.n_cell = 64 64 64

diff --git a/examples/epac2004_benchmarks/run_bithermal.py b/examples/epac2004_benchmarks/run_bithermal.py
@@ -14,7 +14,7 @@
 # sim.n_cell = [128, 128, 128]  # full resolution
 sim.n_cell = [64, 64, 64]
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.dynamic_size = True
 sim.prob_relative = [3.0]
 

diff --git a/examples/epac2004_benchmarks/run_fodo_rf_SC.py b/examples/epac2004_benchmarks/run_fodo_rf_SC.py
@@ -13,7 +13,7 @@
 # set numerical parameters and IO control
 sim.n_cell = [56, 56, 64]
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.dynamic_size = True
 sim.prob_relative = [4.0]
 

diff --git a/examples/epac2004_benchmarks/run_thermal.py b/examples/epac2004_benchmarks/run_thermal.py
@@ -13,7 +13,7 @@
 # set numerical parameters and IO control
 sim.n_cell = [56, 56, 64]
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.dynamic_size = True
 sim.prob_relative = [4.0]
 

diff --git a/examples/expanding_beam/input_expanding_fft.in b/examples/expanding_beam/input_expanding_fft.in
@@ -32,7 +32,7 @@ monitor.backend = h5
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 algo.poisson_solver = "fft"
 
 # Space charge solver with one MR level

diff --git a/examples/expanding_beam/input_expanding_mlmg.in b/examples/expanding_beam/input_expanding_mlmg.in
@@ -32,7 +32,7 @@ monitor.backend = h5
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 # Space charge solver with one MR level
 amr.max_level = 1

diff --git a/examples/expanding_beam/run_expanding_fft.py b/examples/expanding_beam/run_expanding_fft.py
@@ -18,7 +18,7 @@
 sim.blocking_factor_z = [4]
 
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.poisson_solver = "fft"
 sim.dynamic_size = True
 sim.prob_relative = [1.2, 1.1]

diff --git a/examples/expanding_beam/run_expanding_mlmg.py b/examples/expanding_beam/run_expanding_mlmg.py
@@ -18,7 +18,7 @@
 sim.blocking_factor_z = [4]
 
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.dynamic_size = True
 sim.prob_relative = [3.0, 1.1]
 

diff --git a/examples/kurth/input_kurth_10nC_periodic.in b/examples/kurth/input_kurth_10nC_periodic.in
@@ -40,7 +40,7 @@ constf1.kt = 0.7
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 amr.n_cell = 48 48 40
 #amr.n_cell = 72 72 72  # optional for increased precision

diff --git a/examples/kurth/run_kurth_10nC_periodic.py b/examples/kurth/run_kurth_10nC_periodic.py
@@ -13,7 +13,7 @@
 # set numerical parameters and IO control
 sim.n_cell = [48, 48, 40]  # use [72, 72, 72] for increased precision
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 # sim.diagnostics = False  # benchmarking
 sim.slice_step_diagnostics = True
 

diff --git a/examples/linac_segment/input_linac_segment.in b/examples/linac_segment/input_linac_segment.in
@@ -359,7 +359,7 @@ RF1b.sin_coefficients =             \
 # Algorithms
 ###############################################################################
 algo.particle_shape = 2
-algo.space_charge = true
+algo.space_charge = 3D
 
 # Space charge using IGF solver
 algo.poisson_solver = "fft"

diff --git a/examples/linac_segment/run_linac_segment.py b/examples/linac_segment/run_linac_segment.py
@@ -17,7 +17,7 @@
 # sim.n_cell = [64, 64, 64]  #use this for high-resolution runs
 sim.n_cell = [32, 32, 32]
 sim.particle_shape = 2  # B-spline order
-sim.space_charge = True
+sim.space_charge = "3D"
 sim.poisson_solver = "fft"
 sim.dynamic_size = True
 sim.prob_relative = [1.1, 1.1]