From 0f1428e21d0bf7c3cc389009efa9c66f4bc030ab Mon Sep 17 00:00:00 2001 From: GitHub CI Documentation builder Date: Tue, 22 Oct 2024 15:28:30 +0000 Subject: [PATCH] Update docs --- ...__second__order__explicit_8hpp_source.html | 289 +++++++++--------- classBslExplicitPredCorrRTheta-members.html | 4 +- classBslExplicitPredCorrRTheta.html | 12 +- classBslExplicitPredCorrRTheta.js | 4 +- classITimeSolverRTheta.html | 2 +- navtreeindex0.js | 4 +- search/all_e.js | 2 +- search/functions_e.js | 2 +- 8 files changed, 159 insertions(+), 160 deletions(-) diff --git a/bsl__predcorr__second__order__explicit_8hpp_source.html b/bsl__predcorr__second__order__explicit_8hpp_source.html index e089ea08d..e101434d3 100644 --- a/bsl__predcorr__second__order__explicit_8hpp_source.html +++ b/bsl__predcorr__second__order__explicit_8hpp_source.html @@ -176,170 +176,169 @@
133  }
134 
135 
-
136  ~BslExplicitPredCorrRTheta() {};
+
136  ~BslExplicitPredCorrRTheta() override {}
137 
138 
139 
-
140  host_t<DFieldRTheta> operator()(
+
140  host_t<DFieldRTheta> operator()(
141  host_t<DFieldRTheta> allfdistribu,
142  double const dt,
-
143  int const steps) const
-
144  {
-
145  std::chrono::time_point<std::chrono::system_clock> start_time
-
146  = std::chrono::system_clock::now();
-
147  std::chrono::time_point<std::chrono::system_clock> end_time;
-
148 
-
149  // Grid. ------------------------------------------------------------------------------------------
-
150  IdxRangeRTheta const grid(get_idx_range<GridR, GridTheta>(allfdistribu));
-
151 
-
152  host_t<FieldMemRTheta<CoordRTheta>> coords(grid);
-
153  ddc::for_each(grid, [&](IdxRTheta const irp) { coords(irp) = ddc::coordinate(irp); });
-
154 
-
155  IdxRangeBSR radial_bsplines(ddc::discrete_space<BSplinesR>().full_domain().remove_first(
-
156  IdxStep<BSplinesR> {PolarBSplinesRTheta::continuity + 1}));
-
157  IdxRangeBSTheta polar_idx_range(ddc::discrete_space<BSplinesTheta>().full_domain());
-
158 
-
159  // --- Electrostatic potential (phi). -------------------------------------------------------------
-
160  host_t<DFieldMemRTheta> electrical_potential(grid);
-
161 
-
162  SplinePolar electrostatic_potential_coef(
-
163  PolarBSplinesRTheta::singular_idx_range<PolarBSplinesRTheta>(),
-
164  IdxRangeBSRTheta(radial_bsplines, polar_idx_range));
-
165 
-
166  ddc::NullExtrapolationRule extrapolation_rule;
-
167  PolarSplineEvaluator<PolarBSplinesRTheta, ddc::NullExtrapolationRule>
-
168  polar_spline_evaluator(extrapolation_rule);
-
169 
-
170  // --- For the computation of advection field from the electrostatic potential (phi): -------------
-
171  host_t<DVectorFieldMemRTheta<X, Y>> electric_field_alloc(grid);
-
172  host_t<DVectorFieldMemRTheta<X, Y>> electric_field_predicted_alloc(grid);
-
173  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_alloc(grid);
-
174  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_predicted_alloc(grid);
-
175 
-
176  host_t<DVectorFieldRTheta<X, Y>> electric_field(electric_field_alloc);
-
177  host_t<DVectorFieldRTheta<X, Y>> electric_field_predicted(electric_field_predicted_alloc);
-
178  host_t<DVectorFieldRTheta<X, Y>> advection_field(advection_field_alloc);
-
179  host_t<DVectorFieldRTheta<X, Y>> advection_field_predicted(advection_field_predicted_alloc);
-
180 
-
181  AdvectionFieldFinder advection_field_computer(m_mapping);
+
143  int const steps) const final
+
144  {
+
145  std::chrono::time_point<std::chrono::system_clock> start_time;
+
146  std::chrono::time_point<std::chrono::system_clock> end_time;
+
147 
+
148  // Grid. ------------------------------------------------------------------------------------------
+
149  IdxRangeRTheta const grid(get_idx_range<GridR, GridTheta>(allfdistribu));
+
150 
+
151  host_t<FieldMemRTheta<CoordRTheta>> coords(grid);
+
152  ddc::for_each(grid, [&](IdxRTheta const irp) { coords(irp) = ddc::coordinate(irp); });
+
153 
+
154  IdxRangeBSR radial_bsplines(ddc::discrete_space<BSplinesR>().full_domain().remove_first(
+
155  IdxStep<BSplinesR> {PolarBSplinesRTheta::continuity + 1}));
+
156  IdxRangeBSTheta polar_idx_range(ddc::discrete_space<BSplinesTheta>().full_domain());
+
157 
+
158  // --- Electrostatic potential (phi). -------------------------------------------------------------
+
159  host_t<DFieldMemRTheta> electrical_potential(grid);
+
160 
+
161  SplinePolar electrostatic_potential_coef(
+
162  PolarBSplinesRTheta::singular_idx_range<PolarBSplinesRTheta>(),
+
163  IdxRangeBSRTheta(radial_bsplines, polar_idx_range));
+
164 
+
165  ddc::NullExtrapolationRule extrapolation_rule;
+
166  PolarSplineEvaluator<PolarBSplinesRTheta, ddc::NullExtrapolationRule>
+
167  polar_spline_evaluator(extrapolation_rule);
+
168 
+
169  // --- For the computation of advection field from the electrostatic potential (phi): -------------
+
170  host_t<DVectorFieldMemRTheta<X, Y>> electric_field_alloc(grid);
+
171  host_t<DVectorFieldMemRTheta<X, Y>> electric_field_predicted_alloc(grid);
+
172  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_alloc(grid);
+
173  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_predicted_alloc(grid);
+
174 
+
175  host_t<DVectorFieldRTheta<X, Y>> electric_field(electric_field_alloc);
+
176  host_t<DVectorFieldRTheta<X, Y>> electric_field_predicted(electric_field_predicted_alloc);
+
177  host_t<DVectorFieldRTheta<X, Y>> advection_field(advection_field_alloc);
+
178  host_t<DVectorFieldRTheta<X, Y>> advection_field_predicted(advection_field_predicted_alloc);
+
179 
+
180  AdvectionFieldFinder advection_field_computer(m_mapping);
+
181 
182 
183 
-
184 
-
185  // --- Parameter for linearisation of advection field: --------------------------------------------
-
186  start_time = std::chrono::system_clock::now();
-
187  for (int iter(0); iter < steps; ++iter) {
-
188  double const time = iter * dt;
-
189  // STEP 1: From rho^n, we compute phi^n: Poisson equation
-
190  host_t<Spline2DMem> allfdistribu_coef(get_spline_idx_range(m_builder));
-
191  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu));
-
192  PoissonLikeRHSFunction const
-
193  charge_density_coord_1(get_const_field(allfdistribu_coef), m_evaluator);
-
194  m_poisson_solver(charge_density_coord_1, electrostatic_potential_coef);
-
195 
-
196  polar_spline_evaluator(
-
197  get_field(electrical_potential),
-
198  get_const_field(coords),
-
199  electrostatic_potential_coef);
-
200 
-
201  ddc::PdiEvent("iteration")
-
202  .with("iter", iter)
-
203  .and_with("time", time)
-
204  .and_with("density", allfdistribu)
-
205  .and_with("electrical_potential", electrical_potential);
-
206 
-
207  // STEP 2: From phi^n, we compute A^n:
-
208  advection_field_computer(electrostatic_potential_coef, advection_field);
+
184  // --- Parameter for linearisation of advection field: --------------------------------------------
+
185  start_time = std::chrono::system_clock::now();
+
186  for (int iter(0); iter < steps; ++iter) {
+
187  double const time = iter * dt;
+
188  // STEP 1: From rho^n, we compute phi^n: Poisson equation
+
189  host_t<Spline2DMem> allfdistribu_coef(get_spline_idx_range(m_builder));
+
190  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu));
+
191  PoissonLikeRHSFunction const
+
192  charge_density_coord_1(get_const_field(allfdistribu_coef), m_evaluator);
+
193  m_poisson_solver(charge_density_coord_1, electrostatic_potential_coef);
+
194 
+
195  polar_spline_evaluator(
+
196  get_field(electrical_potential),
+
197  get_const_field(coords),
+
198  electrostatic_potential_coef);
+
199 
+
200  ddc::PdiEvent("iteration")
+
201  .with("iter", iter)
+
202  .and_with("time", time)
+
203  .and_with("density", allfdistribu)
+
204  .and_with("electrical_potential", electrical_potential);
+
205 
+
206  // STEP 2: From phi^n, we compute A^n:
+
207  advection_field_computer(electrostatic_potential_coef, advection_field);
+
208 
209 
-
210 
-
211  // STEP 3: From rho^n and A^n, we compute rho^P: Vlasov equation
-
212  // --- Copy rho^n because it will be modified:
-
213  host_t<DFieldMemRTheta> allfdistribu_predicted(grid);
-
214  ddc::parallel_deepcopy(get_field(allfdistribu_predicted), allfdistribu);
-
215  m_advection_solver(get_field(allfdistribu_predicted), get_field(advection_field), dt);
-
216 
-
217  // --- advect also the feet because it is needed for the next step
-
218  host_t<FieldMemRTheta<CoordRTheta>> feet_coords(grid);
-
219  ddc::for_each(grid, [&](IdxRTheta const irp) {
-
220  feet_coords(irp) = CoordRTheta(ddc::coordinate(irp));
-
221  });
-
222  m_find_feet(get_field(feet_coords), get_field(advection_field), dt);
+
210  // STEP 3: From rho^n and A^n, we compute rho^P: Vlasov equation
+
211  // --- Copy rho^n because it will be modified:
+
212  host_t<DFieldMemRTheta> allfdistribu_predicted(grid);
+
213  ddc::parallel_deepcopy(get_field(allfdistribu_predicted), allfdistribu);
+
214  m_advection_solver(get_field(allfdistribu_predicted), get_field(advection_field), dt);
+
215 
+
216  // --- advect also the feet because it is needed for the next step
+
217  host_t<FieldMemRTheta<CoordRTheta>> feet_coords(grid);
+
218  ddc::for_each(grid, [&](IdxRTheta const irp) {
+
219  feet_coords(irp) = CoordRTheta(ddc::coordinate(irp));
+
220  });
+
221  m_find_feet(get_field(feet_coords), get_field(advection_field), dt);
+
222 
223 
-
224 
-
225  // STEP 4: From rho^P, we compute phi^P: Poisson equation
-
226  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu));
-
227  PoissonLikeRHSFunction const
-
228  charge_density_coord_4(get_const_field(allfdistribu_coef), m_evaluator);
-
229  m_poisson_solver(charge_density_coord_4, electrostatic_potential_coef);
-
230 
-
231  // STEP 5: From phi^P, we compute A^P:
-
232  advection_field_computer(electrostatic_potential_coef, advection_field_predicted);
+
224  // STEP 4: From rho^P, we compute phi^P: Poisson equation
+
225  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu_predicted));
+
226  PoissonLikeRHSFunction const
+
227  charge_density_coord_4(get_const_field(allfdistribu_coef), m_evaluator);
+
228  m_poisson_solver(charge_density_coord_4, electrostatic_potential_coef);
+
229 
+
230  // STEP 5: From phi^P, we compute A^P:
+
231  advection_field_computer(electrostatic_potential_coef, advection_field_predicted);
+
232 
233 
-
234 
-
235  // --- we evaluate the advection field A^n at the characteristic feet X^Theta
-
236  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_evaluated(grid);
-
237  host_t<VectorSplineCoeffsMem2D<X, Y>> advection_field_coefs(
-
238  get_spline_idx_range(m_builder));
-
239 
-
240  m_builder(
-
241  ddcHelper::get<X>(advection_field_coefs),
-
242  ddcHelper::get<X>(get_const_field(advection_field)));
-
243  m_builder(
-
244  ddcHelper::get<Y>(advection_field_coefs),
-
245  ddcHelper::get<Y>(get_const_field(advection_field)));
-
246 
-
247  m_evaluator(
-
248  get_field(ddcHelper::get<X>(advection_field_evaluated)),
-
249  get_const_field(feet_coords),
-
250  ddcHelper::get<X>(get_const_field(advection_field_coefs)));
-
251  m_evaluator(
-
252  get_field(ddcHelper::get<Y>(advection_field_evaluated)),
-
253  get_const_field(feet_coords),
-
254  ddcHelper::get<Y>(get_const_field(advection_field_coefs)));
+
234  // --- we evaluate the advection field A^n at the characteristic feet X^P
+
235  host_t<DVectorFieldMemRTheta<X, Y>> advection_field_evaluated(grid);
+
236  host_t<VectorSplineCoeffsMem2D<X, Y>> advection_field_coefs(
+
237  get_spline_idx_range(m_builder));
+
238 
+
239  m_builder(
+
240  ddcHelper::get<X>(advection_field_coefs),
+
241  ddcHelper::get<X>(get_const_field(advection_field)));
+
242  m_builder(
+
243  ddcHelper::get<Y>(advection_field_coefs),
+
244  ddcHelper::get<Y>(get_const_field(advection_field)));
+
245 
+
246  m_evaluator(
+
247  get_field(ddcHelper::get<X>(advection_field_evaluated)),
+
248  get_const_field(feet_coords),
+
249  ddcHelper::get<X>(get_const_field(advection_field_coefs)));
+
250  m_evaluator(
+
251  get_field(ddcHelper::get<Y>(advection_field_evaluated)),
+
252  get_const_field(feet_coords),
+
253  ddcHelper::get<Y>(get_const_field(advection_field_coefs)));
+
254 
255 
-
256 
-
257  // STEP 6: From rho^n and (A^n(X^P) + A^P(X^n))/2, we compute rho^{n+1}: Vlasov equation
-
258  ddc::for_each(grid, [&](IdxRTheta const irp) {
-
259  ddcHelper::get<X>(advection_field)(irp)
-
260  = (ddcHelper::get<X>(advection_field_evaluated)(irp)
-
261  + ddcHelper::get<X>(advection_field_predicted)(irp))
-
262  / 2.;
-
263  ddcHelper::get<Y>(advection_field)(irp)
-
264  = (ddcHelper::get<Y>(advection_field_evaluated)(irp)
-
265  + ddcHelper::get<Y>(advection_field_predicted)(irp))
-
266  / 2.;
-
267  });
+
256  // STEP 6: From rho^n and (A^n(X^P) + A^P(X^n))/2, we compute rho^{n+1}: Vlasov equation
+
257  ddc::for_each(grid, [&](IdxRTheta const irp) {
+
258  ddcHelper::get<X>(advection_field)(irp)
+
259  = (ddcHelper::get<X>(advection_field_evaluated)(irp)
+
260  + ddcHelper::get<X>(advection_field_predicted)(irp))
+
261  / 2.;
+
262  ddcHelper::get<Y>(advection_field)(irp)
+
263  = (ddcHelper::get<Y>(advection_field_evaluated)(irp)
+
264  + ddcHelper::get<Y>(advection_field_predicted)(irp))
+
265  / 2.;
+
266  });
+
267 
268 
-
269 
-
270  m_advection_solver(allfdistribu, get_field(advection_field), dt);
-
271  }
-
272 
-
273  // STEP 1: From rho^n, we compute phi^n: Poisson equation
-
274  host_t<Spline2DMem> allfdistribu_coef(get_spline_idx_range(m_builder));
-
275  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu));
-
276  PoissonLikeRHSFunction const
-
277  charge_density_coord(get_const_field(allfdistribu_coef), m_evaluator);
-
278  m_poisson_solver(charge_density_coord, coords, electrical_potential);
-
279 
-
280  ddc::PdiEvent("last_iteration")
-
281  .with("iter", steps)
-
282  .and_with("time", steps * dt)
-
283  .and_with("density", allfdistribu)
-
284  .and_with("electrical_potential", electrical_potential);
+
269  m_advection_solver(allfdistribu, get_field(advection_field), dt);
+
270  }
+
271 
+
272  // STEP 1: From rho^n, we compute phi^n: Poisson equation
+
273  host_t<Spline2DMem> allfdistribu_coef(get_spline_idx_range(m_builder));
+
274  m_builder(get_field(allfdistribu_coef), get_const_field(allfdistribu));
+
275  PoissonLikeRHSFunction const
+
276  charge_density_coord(get_const_field(allfdistribu_coef), m_evaluator);
+
277  m_poisson_solver(charge_density_coord, coords, electrical_potential);
+
278 
+
279  ddc::PdiEvent("last_iteration")
+
280  .with("iter", steps)
+
281  .and_with("time", steps * dt)
+
282  .and_with("density", allfdistribu)
+
283  .and_with("electrical_potential", electrical_potential);
+
284 
285 
-
286 
-
287  end_time = std::chrono::system_clock::now();
-
288  display_time_difference("Iterations time: ", start_time, end_time);
+
286  end_time = std::chrono::system_clock::now();
+
287  display_time_difference("Iterations time: ", start_time, end_time);
+
288 
289 
-
290 
-
291  return allfdistribu;
-
292  }
-
293 };
+
290  return allfdistribu;
+
291  }
+
292 };
Define a domain for the advection.
Definition: advection_domain.hpp:40
Solve the Poisson-like equation and return the electric field for the coupled Vlasov equation.
Definition: advection_field_rp.hpp:91
Define an advection operator on 2D index range.
Definition: bsl_advection_rp.hpp:60
A second order explicit predictor-corrector for the Vlasov-Poisson equations.
Definition: bsl_predcorr_second_order_explicit.hpp:66
-
host_t< DFieldRTheta > operator()(host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) const
Solves on the equations system.
Definition: bsl_predcorr_second_order_explicit.hpp:140
BslExplicitPredCorrRTheta(AdvectionDomain const &advection_domain, Mapping const &mapping, BslAdvectionRTheta< SplineFootFinder< EulerMethod, AdvectionDomain >, Mapping > &advection_solver, IdxRangeRTheta const &grid, SplineRThetaBuilder const &builder, SplineRThetaEvaluatorNullBound const &rhs_evaluator, PolarSplineFEMPoissonLikeSolver const &poisson_solver, SplineRThetaEvaluatorConstBound const &advection_evaluator)
Instantiate a BslExplicitPredCorrRTheta.
Definition: bsl_predcorr_second_order_explicit.hpp:114
+
host_t< DFieldRTheta > operator()(host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) const final
Solves on the equations system.
Definition: bsl_predcorr_second_order_explicit.hpp:140
A class for describing the circular 2D mapping.
Definition: circular_to_cartesian.hpp:44
A class which provides an implementation of an explicit Euler method.
Definition: euler.hpp:33
Base class for the time solvers.
Definition: itimesolver.hpp:11
diff --git a/classBslExplicitPredCorrRTheta-members.html b/classBslExplicitPredCorrRTheta-members.html index fb7c7ccb0..caacaa102 100644 --- a/classBslExplicitPredCorrRTheta-members.html +++ b/classBslExplicitPredCorrRTheta-members.html @@ -108,8 +108,8 @@ - - + +
BslExplicitPredCorrRTheta(AdvectionDomain const &advection_domain, Mapping const &mapping, BslAdvectionRTheta< SplineFootFinder< EulerMethod, AdvectionDomain >, Mapping > &advection_solver, IdxRangeRTheta const &grid, SplineRThetaBuilder const &builder, SplineRThetaEvaluatorNullBound const &rhs_evaluator, PolarSplineFEMPoissonLikeSolver const &poisson_solver, SplineRThetaEvaluatorConstBound const &advection_evaluator)BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >inline
display_time_difference(std::string const &title, std::chrono::time_point< std::chrono::system_clock > const &start_time, std::chrono::time_point< std::chrono::system_clock > const &end_time) constITimeSolverRThetainlineprotected
operator()(host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) constBslExplicitPredCorrRTheta< Mapping, AdvectionDomain >inlinevirtual
~BslExplicitPredCorrRTheta() (defined in BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >)BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >inline
operator()(host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) const finalBslExplicitPredCorrRTheta< Mapping, AdvectionDomain >inlinevirtual
~BslExplicitPredCorrRTheta() override (defined in BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >)BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >inline
~ITimeSolverRTheta()=default (defined in ITimeSolverRTheta)ITimeSolverRThetavirtual
diff --git a/classBslExplicitPredCorrRTheta.html b/classBslExplicitPredCorrRTheta.html index 63f1c1f26..364116a6a 100644 --- a/classBslExplicitPredCorrRTheta.html +++ b/classBslExplicitPredCorrRTheta.html @@ -124,9 +124,9 @@  BslExplicitPredCorrRTheta (AdvectionDomain const &advection_domain, Mapping const &mapping, BslAdvectionRTheta< SplineFootFinder< EulerMethod, AdvectionDomain >, Mapping > &advection_solver, IdxRangeRTheta const &grid, SplineRThetaBuilder const &builder, SplineRThetaEvaluatorNullBound const &rhs_evaluator, PolarSplineFEMPoissonLikeSolver const &poisson_solver, SplineRThetaEvaluatorConstBound const &advection_evaluator)  Instantiate a BslExplicitPredCorrRTheta. More...
  -host_t< DFieldRTheta > operator() (host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) const - Solves on \( T = dt*N \) the equations system. More...
-  +host_t< DFieldRTheta > operator() (host_t< DFieldRTheta > allfdistribu, double const dt, int const steps) const final + Solves on \( T = dt*N \) the equations system. More...
+  @@ -260,8 +260,8 @@

Member Function Documentation

- -

◆ operator()()

+ +

◆ operator()()

Additional Inherited Members

diff --git a/classBslExplicitPredCorrRTheta.js b/classBslExplicitPredCorrRTheta.js index 92b5b0cd4..b864e972d 100644 --- a/classBslExplicitPredCorrRTheta.js +++ b/classBslExplicitPredCorrRTheta.js @@ -1,6 +1,6 @@ var classBslExplicitPredCorrRTheta = [ [ "BslExplicitPredCorrRTheta", "classBslExplicitPredCorrRTheta.html#a798b7348c59ee58fb5bdc09d2792b6cc", null ], - [ "~BslExplicitPredCorrRTheta", "classBslExplicitPredCorrRTheta.html#ab5b5e97a788d1556035afad5cdffb4db", null ], - [ "operator()", "classBslExplicitPredCorrRTheta.html#a4a0d13a36c04660e9416fd8dba361e43", null ] + [ "~BslExplicitPredCorrRTheta", "classBslExplicitPredCorrRTheta.html#a26b8afb30dc2978dab211c9b8cab1508", null ], + [ "operator()", "classBslExplicitPredCorrRTheta.html#aaf7de730188384e04d3121a0aab47d95", null ] ]; \ No newline at end of file diff --git a/classITimeSolverRTheta.html b/classITimeSolverRTheta.html index 86d4980df..6f4157f70 100644 --- a/classITimeSolverRTheta.html +++ b/classITimeSolverRTheta.html @@ -188,7 +188,7 @@

Returns
A Field toward allfdistribu.
-

Implemented in BslImplicitPredCorrRTheta< Mapping, AdvectionDomain >, BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >, and BslPredCorrRTheta< Mapping, FootFinder >.

+

Implemented in BslExplicitPredCorrRTheta< Mapping, AdvectionDomain >, BslImplicitPredCorrRTheta< Mapping, AdvectionDomain >, and BslPredCorrRTheta< Mapping, FootFinder >.

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