libMesh::Euler2Solver Class Reference

#include <euler2_solver.h>

Inheritance diagram for libMesh::Euler2Solver:

Public Types

typedef FirstOrderUnsteadySolver Parent
 
typedef DifferentiableSystem sys_type
 

Public Member Functions

 Euler2Solver (sys_type &s)
 
virtual ~Euler2Solver ()
 
virtual Real error_order () const libmesh_override
 
virtual bool element_residual (bool request_jacobian, DiffContext &) libmesh_override
 
virtual bool side_residual (bool request_jacobian, DiffContext &) libmesh_override
 
virtual bool nonlocal_residual (bool request_jacobian, DiffContext &) libmesh_override
 
virtual unsigned int time_order () const libmesh_override
 
virtual void init () libmesh_override
 
virtual void init_data () libmesh_override
 
virtual void reinit () libmesh_override
 
virtual void solve () libmesh_override
 
virtual void advance_timestep () libmesh_override
 
virtual void adjoint_advance_timestep () libmesh_override
 
virtual void retrieve_timestep () libmesh_override
 
Number old_nonlinear_solution (const dof_id_type global_dof_number) const
 
virtual Real du (const SystemNorm &norm) const libmesh_override
 
virtual bool is_steady () const libmesh_override
 
virtual void before_timestep ()
 
const sys_typesystem () const
 
sys_typesystem ()
 
virtual UniquePtr< DiffSolver > & diff_solver ()
 
virtual UniquePtr< LinearSolver< Number > > & linear_solver ()
 
void set_solution_history (const SolutionHistory &_solution_history)
 
bool is_adjoint () const
 
void set_is_adjoint (bool _is_adjoint_value)
 

Static Public Member Functions

static std::string get_info ()
 
static void print_info (std::ostream &out=libMesh::out)
 
static unsigned int n_objects ()
 
static void enable_print_counter_info ()
 
static void disable_print_counter_info ()
 

Public Attributes

Real theta
 
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
 
bool quiet
 
unsigned int reduce_deltat_on_diffsolver_failure
 

Protected Types

typedef bool(DifferentiablePhysics::* ResFuncType) (bool, DiffContext &)
 
typedef void(DiffContext::* ReinitFuncType) (Real)
 
typedef std::map< std::string, std::pair< unsigned int, unsigned int > > Counts
 

Protected Member Functions

virtual bool _general_residual (bool request_jacobian, DiffContext &, ResFuncType mass, ResFuncType damping, ResFuncType time_deriv, ResFuncType constraint, ReinitFuncType reinit, bool compute_second_order_eqns)
 
void prepare_accel (DiffContext &context)
 
bool compute_second_order_eqns (bool compute_jacobian, DiffContext &c)
 
void increment_constructor_count (const std::string &name)
 
void increment_destructor_count (const std::string &name)
 

Protected Attributes

bool first_solve
 
bool first_adjoint_step
 
UniquePtr< DiffSolver_diff_solver
 
UniquePtr< LinearSolver< Number > > _linear_solver
 
sys_type_system
 
UniquePtr< SolutionHistorysolution_history
 

Static Protected Attributes

static Counts _counts
 
static Threads::atomic< unsigned int > _n_objects
 
static Threads::spin_mutex _mutex
 
static bool _enable_print_counter = true
 

Detailed Description

This class defines a theta-method (defaulting to Backward Euler with theta = 1.0) solver to handle time integration of DifferentiableSystems. The "Euler2" solver differs from Euler in how it evaluates residuals at intermediate theta values: Euler solves m(u,u') = f(theta*u_new + (1-theta)*u_old), Euler2 solves m(u') = theta*f(u_new) + (1-theta)*f(u_old) i.e. the trapezoidal rule for theta = 0.5

This class is part of the new DifferentiableSystem framework, which is still experimental. Users of this framework should beware of bugs and future API changes.

Author
Roy H. Stogner
Date
2006

Definition at line 48 of file euler2_solver.h.

Member Typedef Documentation

typedef std::map<std::string, std::pair<unsigned int, unsigned int> > libMesh::ReferenceCounter::Counts
protectedinherited

Data structure to log the information. The log is identified by the class name.

Definition at line 119 of file reference_counter.h.

The parent class

Definition at line 54 of file euler2_solver.h.

typedef void(DiffContext::* libMesh::TimeSolver::ReinitFuncType) (Real)
protectedinherited

Definition at line 272 of file time_solver.h.

typedef bool(DifferentiablePhysics::* libMesh::TimeSolver::ResFuncType) (bool, DiffContext &)
protectedinherited

Definitions of argument types for use in refactoring subclasses.

Definition at line 270 of file time_solver.h.

The type of system

Definition at line 64 of file time_solver.h.

Constructor & Destructor Documentation

libMesh::Euler2Solver::Euler2Solver ( sys_type s)
explicit

Constructor. Requires a reference to the system to be solved.

Definition at line 27 of file euler2_solver.C.

libMesh::Euler2Solver::~Euler2Solver ( )
virtual

Destructor.

Definition at line 34 of file euler2_solver.C.

35 {
36 }

Member Function Documentation

bool libMesh::Euler2Solver::_general_residual ( bool  request_jacobian,
DiffContext context,
ResFuncType  mass,
ResFuncType  damping,
ResFuncType  time_deriv,
ResFuncType  constraint,
ReinitFuncType  reinit,
bool  compute_second_order_eqns 
)
protectedvirtual

This method is the underlying implementation of the public residual methods.

Definition at line 99 of file euler2_solver.C.

References libMesh::TimeSolver::_system, libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), libMesh::DifferentiableSystem::deltat, libMesh::DiffContext::elem_solution_derivative, libMesh::DiffContext::elem_solution_rate_derivative, libMesh::DiffContext::fixed_solution_derivative, libMesh::DiffContext::get_dof_indices(), libMesh::DiffContext::get_elem_fixed_solution(), libMesh::DiffContext::get_elem_jacobian(), libMesh::DiffContext::get_elem_residual(), libMesh::DiffContext::get_elem_solution(), libMesh::DiffContext::get_elem_solution_rate(), libMesh::DifferentiableSystem::get_physics(), libMesh::UnsteadySolver::old_nonlinear_solution(), libMesh::FirstOrderUnsteadySolver::prepare_accel(), libMesh::DenseVector< T >::size(), libMesh::DenseVector< T >::swap(), libMesh::DenseMatrix< T >::swap(), theta, and libMesh::System::use_fixed_solution.

Referenced by element_residual(), nonlocal_residual(), and side_residual().

107 {
108  unsigned int n_dofs = context.get_elem_solution().size();
109 
110  // Local nonlinear solution at old timestep
111  DenseVector<Number> old_elem_solution(n_dofs);
112  for (unsigned int i=0; i != n_dofs; ++i)
113  old_elem_solution(i) =
114  old_nonlinear_solution(context.get_dof_indices()[i]);
115 
116  // Local time derivative of solution
117  context.get_elem_solution_rate() = context.get_elem_solution();
118  context.get_elem_solution_rate() -= old_elem_solution;
119  context.elem_solution_rate_derivative = 1 / _system.deltat;
120  context.get_elem_solution_rate() *=
121  context.elem_solution_rate_derivative;
122 
123  // Our first evaluations are at the final elem_solution
124  context.elem_solution_derivative = 1.0;
125 
126  // If a fixed solution is requested, we'll use the elem_solution
127  // at the new timestep
128  // FIXME - should this be the theta solution instead?
130  context.get_elem_fixed_solution() = context.get_elem_solution();
131 
132  context.fixed_solution_derivative = 1.0;
133 
134  // We need to save the old jacobian and old residual since we'll be
135  // multiplying some of the new contributions by theta or 1-theta
136  DenseMatrix<Number> old_elem_jacobian(n_dofs, n_dofs);
137  DenseVector<Number> old_elem_residual(n_dofs);
138  old_elem_residual.swap(context.get_elem_residual());
139  if (request_jacobian)
140  old_elem_jacobian.swap(context.get_elem_jacobian());
141 
142  // Local time derivative of solution
143  context.get_elem_solution_rate() = context.get_elem_solution();
144  context.get_elem_solution_rate() -= old_elem_solution;
145  context.elem_solution_rate_derivative = 1 / _system.deltat;
146  context.get_elem_solution_rate() *=
147  context.elem_solution_rate_derivative;
148 
149  // If we are asked to compute residuals for second order variables,
150  // we also populate the acceleration part so the user can use that.
152  this->prepare_accel(context);
153 
154  // Move the mesh into place first if necessary, set t = t_{n+1}
155  (context.*reinit_func)(1.);
156 
157  // First, evaluate time derivative at the new timestep.
158  // The element should already be in the proper place
159  // even for a moving mesh problem.
160  bool jacobian_computed =
161  (_system.get_physics()->*time_deriv)(request_jacobian, context);
162 
163  // Next, evaluate the mass residual at the new timestep
164 
165  jacobian_computed = (_system.get_physics()->*mass)(jacobian_computed, context) &&
166  jacobian_computed;
167 
168  // If we have second-order variables, we need to get damping terms
169  // and the velocity equations
171  {
172  jacobian_computed = (_system.get_physics()->*damping)(jacobian_computed, context) &&
173  jacobian_computed;
174 
175  jacobian_computed = this->compute_second_order_eqns(jacobian_computed, context) &&
176  jacobian_computed;
177  }
178 
179  // Add the constraint term
180  jacobian_computed = (_system.get_physics()->*constraint)(jacobian_computed, context) &&
181  jacobian_computed;
182 
183  // The new solution's contribution is scaled by theta
184  context.get_elem_residual() *= theta;
185  context.get_elem_jacobian() *= theta;
186 
187  // Save the new solution's term
188  DenseMatrix<Number> elem_jacobian_newterm(n_dofs, n_dofs);
189  DenseVector<Number> elem_residual_newterm(n_dofs);
190  elem_residual_newterm.swap(context.get_elem_residual());
191  if (request_jacobian)
192  elem_jacobian_newterm.swap(context.get_elem_jacobian());
193 
194  // Add the time-dependent term for the old solution
195 
196  // Make sure elem_solution is set up for elem_reinit to use
197  // Move elem_->old_, old_->elem_
198  context.get_elem_solution().swap(old_elem_solution);
199  context.elem_solution_derivative = 0.0;
200 
201  // Move the mesh into place if necessary, set t = t_{n}
202  (context.*reinit_func)(0.);
203 
204  jacobian_computed =
205  (_system.get_physics()->*time_deriv)(jacobian_computed, context) &&
206  jacobian_computed;
207 
208  // Add the mass residual term for the old solution
209 
210  // Evaluating the mass residual at both old and new timesteps will be
211  // redundant in most problems but may be necessary for time accuracy
212  // or stability in moving mesh problems or problems with user-overridden
213  // mass_residual functions
214 
215  jacobian_computed =
216  (_system.get_physics()->*mass)(jacobian_computed, context) &&
217  jacobian_computed;
218 
219  // If we have second-order variables, we need to get damping terms
220  // and the velocity equations
222  {
223  jacobian_computed = (_system.get_physics()->*damping)(jacobian_computed, context) &&
224  jacobian_computed;
225 
226  jacobian_computed = this->compute_second_order_eqns(jacobian_computed, context) &&
227  jacobian_computed;
228  }
229 
230  // The old solution's contribution is scaled by (1-theta)
231  context.get_elem_residual() *= (1-theta);
232  context.get_elem_jacobian() *= (1-theta);
233 
234  // Restore the elem_solution
235  // Move elem_->elem_, old_->old_
236  context.get_elem_solution().swap(old_elem_solution);
237  context.elem_solution_derivative = 1;
238 
239  // Restore the elem position if necessary, set t = t_{n+1}
240  (context.*reinit_func)(1.);
241 
242  // Add back (or restore) the old residual/jacobian
243  context.get_elem_residual() += old_elem_residual;
244  if (request_jacobian)
245  {
246  if (jacobian_computed)
247  context.get_elem_jacobian() += old_elem_jacobian;
248  else
249  context.get_elem_jacobian().swap(old_elem_jacobian);
250  }
251 
252  // Add the saved new-solution terms
253  context.get_elem_residual() += elem_residual_newterm;
254  if (jacobian_computed)
255  context.get_elem_jacobian() += elem_jacobian_newterm;
256 
257  return jacobian_computed;
258 }
bool compute_second_order_eqns(bool compute_jacobian, DiffContext &c)
sys_type & _system
Definition: time_solver.h:257
Number old_nonlinear_solution(const dof_id_type global_dof_number) const
bool use_fixed_solution
Definition: system.h:1491
const DifferentiablePhysics * get_physics() const
Definition: diff_system.h:169
void libMesh::UnsteadySolver::adjoint_advance_timestep ( )
virtualinherited

This method advances the adjoint solution to the previous timestep, after an adjoint_solve() has been performed. This will be done before every UnsteadySolver::adjoint_solve().

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::NewmarkSolver.

Definition at line 178 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::DifferentiableSystem::deltat, libMesh::UnsteadySolver::first_adjoint_step, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::NumericVector< T >::localize(), libMesh::UnsteadySolver::old_local_nonlinear_solution, libMesh::TimeSolver::solution_history, and libMesh::System::time.

179 {
180  // On the first call of this function, we dont save the adjoint solution or
181  // decrement the time, we just call the retrieve function below
182  if (!first_adjoint_step)
183  {
184  // Call the store function to store the last adjoint before decrementing the time
185  solution_history->store();
186  // Decrement the system time
188  }
189  else
190  {
191  first_adjoint_step = false;
192  }
193 
194  // Retrieve the primal solution vectors at this time using the
195  // solution_history object
196  solution_history->retrieve();
197 
198  // Dont forget to localize the old_nonlinear_solution !
199  _system.get_vector("_old_nonlinear_solution").localize
202 }
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
const NumericVector< Number > & get_vector(const std::string &vec_name) const
Definition: system.C:792
UniquePtr< SolutionHistory > solution_history
Definition: time_solver.h:264
const std::vector< dof_id_type > & get_send_list() const
Definition: dof_map.h:394
virtual void localize(std::vector< T > &v_local) const =0
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
void libMesh::UnsteadySolver::advance_timestep ( )
virtualinherited

This method advances the solution to the next timestep, after a solve() has been performed. Often this will be done after every UnsteadySolver::solve(), but adaptive mesh refinement and/or adaptive time step selection may require some solve() steps to be repeated.

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::AdaptiveTimeSolver, and libMesh::NewmarkSolver.

Definition at line 152 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::DifferentiableSystem::deltat, libMesh::UnsteadySolver::first_solve, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::NumericVector< T >::localize(), libMesh::UnsteadySolver::old_local_nonlinear_solution, libMesh::System::solution, libMesh::TimeSolver::solution_history, and libMesh::System::time.

Referenced by libMesh::NewmarkSolver::advance_timestep(), and libMesh::UnsteadySolver::solve().

153 {
154  if (!first_solve)
155  {
156  // Store the solution, does nothing by default
157  // User has to attach appropriate solution_history object for this to
158  // actually store anything anywhere
159  solution_history->store();
160 
162  }
163 
164  NumericVector<Number> & old_nonlinear_soln =
165  _system.get_vector("_old_nonlinear_solution");
166  NumericVector<Number> & nonlinear_solution =
167  *(_system.solution);
168 
169  old_nonlinear_soln = nonlinear_solution;
170 
171  old_nonlinear_soln.localize
174 }
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
UniquePtr< NumericVector< Number > > solution
Definition: system.h:1521
const NumericVector< Number > & get_vector(const std::string &vec_name) const
Definition: system.C:792
UniquePtr< SolutionHistory > solution_history
Definition: time_solver.h:264
const std::vector< dof_id_type > & get_send_list() const
Definition: dof_map.h:394
virtual void localize(std::vector< T > &v_local) const =0
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
virtual void libMesh::TimeSolver::before_timestep ( )
inlinevirtualinherited

This method is for subclasses or users to override to do arbitrary processing between timesteps

Definition at line 166 of file time_solver.h.

166 {}
bool libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns ( bool  compute_jacobian,
DiffContext c 
)
protectedinherited

If there are second order variables, then we need to compute their residual equations and corresponding Jacobian. The residual equation will simply be $ \dot{u} - v = 0 $, where $ u $ is the second order variable add by the user and $ v $ is the variable added by the time-solver as the "velocity" variable.

Definition at line 32 of file first_order_unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::DiffContext::get_dof_indices(), libMesh::DiffContext::get_elem_jacobian(), libMesh::DiffContext::get_elem_residual(), libMesh::DiffContext::get_elem_solution_derivative(), libMesh::DiffContext::get_elem_solution_rate_derivative(), libMesh::FEMContext::get_element_fe(), libMesh::FEMContext::get_element_qrule(), libMesh::DifferentiableSystem::get_second_order_dot_var(), libMesh::DiffContext::get_system(), libMesh::FEMContext::interior_rate(), libMesh::FEMContext::interior_value(), libMesh::DifferentiablePhysics::is_second_order_var(), libMesh::libmesh_assert(), libmesh_nullptr, libMesh::QBase::n_points(), libMesh::DiffContext::n_vars(), libMesh::Variable::type(), and libMesh::System::variable().

Referenced by libMesh::EulerSolver::_general_residual(), _general_residual(), libMesh::EulerSolver::element_residual(), element_residual(), libMesh::EulerSolver::nonlocal_residual(), nonlocal_residual(), and libMesh::FirstOrderUnsteadySolver::time_order().

33 {
34  FEMContext & context = cast_ref<FEMContext &>(c);
35 
36  unsigned int n_qpoints = context.get_element_qrule().n_points();
37 
38  for (unsigned int var = 0; var != context.n_vars(); ++var)
39  {
40  if (!this->_system.is_second_order_var(var))
41  continue;
42 
43  unsigned int dot_var = this->_system.get_second_order_dot_var(var);
44 
45  // We're assuming that the FE space for var and dot_var are the same
46  libmesh_assert( context.get_system().variable(var).type() ==
47  context.get_system().variable(dot_var).type() );
48 
49  FEBase * elem_fe = libmesh_nullptr;
50  context.get_element_fe( var, elem_fe );
51 
52  const std::vector<Real> & JxW = elem_fe->get_JxW();
53 
54  const std::vector<std::vector<Real> > & phi = elem_fe->get_phi();
55 
56  const unsigned int n_dofs = cast_int<unsigned int>
57  (context.get_dof_indices(dot_var).size());
58 
59  DenseSubVector<Number> & Fu = context.get_elem_residual(var);
60  DenseSubMatrix<Number> & Kuu = context.get_elem_jacobian( var, var );
61  DenseSubMatrix<Number> & Kuv = context.get_elem_jacobian( var, dot_var );
62 
63  for (unsigned int qp = 0; qp != n_qpoints; ++qp)
64  {
65  Number udot, v;
66  context.interior_rate(var, qp, udot);
67  context.interior_value(dot_var, qp, v);
68 
69  for (unsigned int i = 0; i < n_dofs; i++)
70  {
71  Fu(i) += JxW[qp]*(udot-v)*phi[i][qp];
72 
73  if (compute_jacobian)
74  {
75  Number rate_factor = JxW[qp]*context.get_elem_solution_rate_derivative()*phi[i][qp];
76  Number soln_factor = JxW[qp]*context.get_elem_solution_derivative()*phi[i][qp];
77 
78  Kuu(i,i) += rate_factor*phi[i][qp];
79  Kuv(i,i) -= soln_factor*phi[i][qp];
80 
81  for (unsigned int j = i+1; j < n_dofs; j++)
82  {
83  Kuu(i,j) += rate_factor*phi[j][qp];
84  Kuu(j,i) += rate_factor*phi[j][qp];
85 
86  Kuv(i,j) -= soln_factor*phi[j][qp];
87  Kuv(j,i) -= soln_factor*phi[j][qp];
88  }
89  }
90  }
91  }
92  }
93 
94  return compute_jacobian;
95 }
const class libmesh_nullptr_t libmesh_nullptr
libmesh_assert(j)
unsigned int get_second_order_dot_var(unsigned int var) const
Definition: diff_system.C:313
sys_type & _system
Definition: time_solver.h:257
FEGenericBase< Real > FEBase
bool is_second_order_var(unsigned int var) const
Definition: diff_physics.h:530
virtual UniquePtr<DiffSolver>& libMesh::TimeSolver::diff_solver ( )
inlinevirtualinherited

An implicit linear or nonlinear solver to use at each timestep.

Reimplemented in libMesh::AdaptiveTimeSolver.

Definition at line 181 of file time_solver.h.

References libMesh::TimeSolver::_diff_solver.

Referenced by libMesh::TimeSolver::init(), libMesh::TimeSolver::init_data(), libMesh::TimeSolver::reinit(), and libMesh::TimeSolver::solve().

181 { return _diff_solver; }
UniquePtr< DiffSolver > _diff_solver
Definition: time_solver.h:247
void libMesh::ReferenceCounter::disable_print_counter_info ( )
staticinherited
Real libMesh::UnsteadySolver::du ( const SystemNorm norm) const
virtualinherited

Computes the size of ||u^{n+1} - u^{n}|| in some norm.

Note
While you can always call this function, its result may or may not be very meaningful. For example, if you call this function right after calling advance_timestep() then you'll get a result of zero since old_nonlinear_solution is set equal to nonlinear_solution in this function.

Implements libMesh::TimeSolver.

Definition at line 227 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::calculate_norm(), libMesh::System::get_vector(), and libMesh::System::solution.

228 {
229 
230  UniquePtr<NumericVector<Number> > solution_copy =
231  _system.solution->clone();
232 
233  solution_copy->add(-1., _system.get_vector("_old_nonlinear_solution"));
234 
235  solution_copy->close();
236 
237  return _system.calculate_norm(*solution_copy, norm);
238 }
sys_type & _system
Definition: time_solver.h:257
UniquePtr< NumericVector< Number > > solution
Definition: system.h:1521
const NumericVector< Number > & get_vector(const std::string &vec_name) const
Definition: system.C:792
Real calculate_norm(const NumericVector< Number > &v, unsigned int var, FEMNormType norm_type, std::set< unsigned int > *skip_dimensions=libmesh_nullptr) const
Definition: system.C:1397
bool libMesh::Euler2Solver::element_residual ( bool  request_jacobian,
DiffContext context 
)
virtual

This method uses the DifferentiablePhysics' element_time_derivative() and element_constraint() to build a full residual on an element. What combination it uses will depend on theta.

Implements libMesh::TimeSolver.

Definition at line 50 of file euler2_solver.C.

References libMesh::DifferentiablePhysics::_eulerian_time_deriv(), _general_residual(), libMesh::TimeSolver::_system, libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), libMesh::DifferentiablePhysics::damping_residual(), libMesh::DiffContext::elem_reinit(), libMesh::DifferentiablePhysics::element_constraint(), libMesh::DifferentiableSystem::get_physics(), libMesh::DifferentiablePhysics::get_second_order_vars(), and libMesh::DifferentiablePhysics::mass_residual().

52 {
54 
55  return this->_general_residual(request_jacobian,
56  context,
62  compute_second_order_eqns);
63 }
const std::set< unsigned int > & get_second_order_vars() const
Definition: diff_physics.h:527
bool compute_second_order_eqns(bool compute_jacobian, DiffContext &c)
virtual bool _general_residual(bool request_jacobian, DiffContext &, ResFuncType mass, ResFuncType damping, ResFuncType time_deriv, ResFuncType constraint, ReinitFuncType reinit, bool compute_second_order_eqns)
Definition: euler2_solver.C:99
virtual bool damping_residual(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:371
virtual void elem_reinit(Real)
Definition: diff_context.h:75
bool _eulerian_time_deriv(bool request_jacobian, DiffContext &)
virtual bool mass_residual(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:315
sys_type & _system
Definition: time_solver.h:257
const DifferentiablePhysics * get_physics() const
Definition: diff_system.h:169
virtual bool element_constraint(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:141
void libMesh::ReferenceCounter::enable_print_counter_info ( )
staticinherited

Methods to enable/disable the reference counter output from print_info()

Definition at line 101 of file reference_counter.C.

References libMesh::ReferenceCounter::_enable_print_counter.

Referenced by libMesh::ReferenceCounter::n_objects().

102 {
103  _enable_print_counter = true;
104  return;
105 }
Real libMesh::Euler2Solver::error_order ( ) const
virtual

Error convergence order: 2 for Crank-Nicolson, 1 otherwise

Implements libMesh::UnsteadySolver.

Definition at line 40 of file euler2_solver.C.

References theta.

41 {
42  if (theta == 0.5)
43  return 2.;
44  return 1.;
45 }
std::string libMesh::ReferenceCounter::get_info ( )
staticinherited

Gets a string containing the reference information.

Definition at line 47 of file reference_counter.C.

References libMesh::ReferenceCounter::_counts, and libMesh::Quality::name().

Referenced by libMesh::ReferenceCounter::print_info().

48 {
49 #if defined(LIBMESH_ENABLE_REFERENCE_COUNTING) && defined(DEBUG)
50 
51  std::ostringstream oss;
52 
53  oss << '\n'
54  << " ---------------------------------------------------------------------------- \n"
55  << "| Reference count information |\n"
56  << " ---------------------------------------------------------------------------- \n";
57 
58  for (Counts::iterator it = _counts.begin();
59  it != _counts.end(); ++it)
60  {
61  const std::string name(it->first);
62  const unsigned int creations = it->second.first;
63  const unsigned int destructions = it->second.second;
64 
65  oss << "| " << name << " reference count information:\n"
66  << "| Creations: " << creations << '\n'
67  << "| Destructions: " << destructions << '\n';
68  }
69 
70  oss << " ---------------------------------------------------------------------------- \n";
71 
72  return oss.str();
73 
74 #else
75 
76  return "";
77 
78 #endif
79 }
std::string name(const ElemQuality q)
Definition: elem_quality.C:39
void libMesh::ReferenceCounter::increment_constructor_count ( const std::string &  name)
inlineprotectedinherited

Increments the construction counter. Should be called in the constructor of any derived class that will be reference counted.

Definition at line 185 of file reference_counter.h.

References libMesh::ReferenceCounter::_counts, libMesh::Quality::name(), and libMesh::Threads::spin_mtx.

Referenced by libMesh::ReferenceCounter::n_objects(), and libMesh::ReferenceCountedObject< RBParametrized >::ReferenceCountedObject().

186 {
187  Threads::spin_mutex::scoped_lock lock(Threads::spin_mtx);
188  std::pair<unsigned int, unsigned int> & p = _counts[name];
189 
190  p.first++;
191 }
std::string name(const ElemQuality q)
Definition: elem_quality.C:39
spin_mutex spin_mtx
Definition: threads.C:29
void libMesh::ReferenceCounter::increment_destructor_count ( const std::string &  name)
inlineprotectedinherited

Increments the destruction counter. Should be called in the destructor of any derived class that will be reference counted.

Definition at line 198 of file reference_counter.h.

References libMesh::ReferenceCounter::_counts, libMesh::Quality::name(), and libMesh::Threads::spin_mtx.

Referenced by libMesh::ReferenceCounter::n_objects(), and libMesh::ReferenceCountedObject< RBParametrized >::~ReferenceCountedObject().

199 {
200  Threads::spin_mutex::scoped_lock lock(Threads::spin_mtx);
201  std::pair<unsigned int, unsigned int> & p = _counts[name];
202 
203  p.second++;
204 }
std::string name(const ElemQuality q)
Definition: elem_quality.C:39
spin_mutex spin_mtx
Definition: threads.C:29
void libMesh::UnsteadySolver::init ( )
virtualinherited

The initialization function. This method is used to initialize internal data structures before a simulation begins.

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::AdaptiveTimeSolver, and libMesh::SecondOrderUnsteadySolver.

Definition at line 46 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::add_vector(), and libMesh::TimeSolver::init().

Referenced by libMesh::SecondOrderUnsteadySolver::init().

47 {
49 
50  _system.add_vector("_old_nonlinear_solution");
51 }
sys_type & _system
Definition: time_solver.h:257
NumericVector< Number > & add_vector(const std::string &vec_name, const bool projections=true, const ParallelType type=PARALLEL)
Definition: system.C:679
virtual void init()
Definition: time_solver.C:64
void libMesh::UnsteadySolver::init_data ( )
virtualinherited

The data initialization function. This method is used to initialize internal data structures after the underlying System has been initialized

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::SecondOrderUnsteadySolver.

Definition at line 55 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::GHOSTED, libMesh::TimeSolver::init_data(), libMesh::System::n_dofs(), libMesh::System::n_local_dofs(), libMesh::UnsteadySolver::old_local_nonlinear_solution, and libMesh::SERIAL.

Referenced by libMesh::SecondOrderUnsteadySolver::init_data().

56 {
58 
59 #ifdef LIBMESH_ENABLE_GHOSTED
62  GHOSTED);
63 #else
65 #endif
66 }
virtual void init_data()
Definition: time_solver.C:77
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
dof_id_type n_local_dofs() const
Definition: system.C:183
dof_id_type n_dofs() const
Definition: system.C:146
const std::vector< dof_id_type > & get_send_list() const
Definition: dof_map.h:394
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
bool libMesh::TimeSolver::is_adjoint ( ) const
inlineinherited

Accessor for querying whether we need to do a primal or adjoint solve

Definition at line 232 of file time_solver.h.

References libMesh::TimeSolver::_is_adjoint.

Referenced by libMesh::FEMSystem::build_context().

233  { return _is_adjoint; }
virtual bool libMesh::UnsteadySolver::is_steady ( ) const
inlinevirtualinherited

This is not a steady-state solver.

Implements libMesh::TimeSolver.

Definition at line 153 of file unsteady_solver.h.

153 { return false; }
virtual UniquePtr<LinearSolver<Number> >& libMesh::TimeSolver::linear_solver ( )
inlinevirtualinherited

An implicit linear solver to use for adjoint and sensitivity problems.

Reimplemented in libMesh::AdaptiveTimeSolver.

Definition at line 186 of file time_solver.h.

References libMesh::TimeSolver::_linear_solver.

Referenced by libMesh::TimeSolver::init(), libMesh::TimeSolver::init_data(), and libMesh::TimeSolver::reinit().

186 { return _linear_solver; }
UniquePtr< LinearSolver< Number > > _linear_solver
Definition: time_solver.h:252
static unsigned int libMesh::ReferenceCounter::n_objects ( )
inlinestaticinherited
bool libMesh::Euler2Solver::nonlocal_residual ( bool  request_jacobian,
DiffContext context 
)
virtual

This method uses the DifferentiablePhysics' nonlocal_time_derivative() and nonlocal_constraint() to build a full residual for non-local terms. What combination it uses will depend on theta.

Implements libMesh::TimeSolver.

Definition at line 82 of file euler2_solver.C.

References _general_residual(), libMesh::TimeSolver::_system, libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), libMesh::DifferentiableSystem::have_second_order_scalar_vars(), libMesh::DifferentiablePhysics::nonlocal_constraint(), libMesh::DifferentiablePhysics::nonlocal_damping_residual(), libMesh::DifferentiablePhysics::nonlocal_mass_residual(), libMesh::DiffContext::nonlocal_reinit(), and libMesh::DifferentiablePhysics::nonlocal_time_derivative().

84 {
86 
87  return this->_general_residual(request_jacobian,
88  context,
94  compute_second_order_eqns);
95 }
bool compute_second_order_eqns(bool compute_jacobian, DiffContext &c)
virtual bool _general_residual(bool request_jacobian, DiffContext &, ResFuncType mass, ResFuncType damping, ResFuncType time_deriv, ResFuncType constraint, ReinitFuncType reinit, bool compute_second_order_eqns)
Definition: euler2_solver.C:99
virtual bool nonlocal_time_derivative(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:208
bool have_second_order_scalar_vars() const
Definition: diff_system.C:348
virtual bool nonlocal_constraint(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:226
sys_type & _system
Definition: time_solver.h:257
virtual bool nonlocal_damping_residual(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:403
virtual bool nonlocal_mass_residual(bool request_jacobian, DiffContext &c)
virtual void nonlocal_reinit(Real)
Definition: diff_context.h:93
Number libMesh::UnsteadySolver::old_nonlinear_solution ( const dof_id_type  global_dof_number) const
inherited
Returns
The old nonlinear solution for the specified global DOF.

Definition at line 216 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), libMesh::DofMap::n_dofs(), and libMesh::UnsteadySolver::old_local_nonlinear_solution.

Referenced by libMesh::EulerSolver::_general_residual(), _general_residual(), and libMesh::NewmarkSolver::_general_residual().

218 {
219  libmesh_assert_less (global_dof_number, _system.get_dof_map().n_dofs());
220  libmesh_assert_less (global_dof_number, old_local_nonlinear_solution->size());
221 
222  return (*old_local_nonlinear_solution)(global_dof_number);
223 }
dof_id_type n_dofs() const
Definition: dof_map.h:510
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
void libMesh::FirstOrderUnsteadySolver::prepare_accel ( DiffContext context)
protectedinherited

If there are second order variables in the system, then we also prepare the accel for those variables so the user can treat them as such.

Definition at line 25 of file first_order_unsteady_solver.C.

References libMesh::DiffContext::elem_solution_accel_derivative, libMesh::DiffContext::get_elem_solution_accel(), libMesh::DiffContext::get_elem_solution_rate(), and libMesh::DiffContext::get_elem_solution_rate_derivative().

Referenced by libMesh::EulerSolver::_general_residual(), _general_residual(), and libMesh::FirstOrderUnsteadySolver::time_order().

26 {
27  context.get_elem_solution_accel() = context.get_elem_solution_rate();
28 
29  context.elem_solution_accel_derivative = context.get_elem_solution_rate_derivative();
30 }
void libMesh::ReferenceCounter::print_info ( std::ostream &  out = libMesh::out)
staticinherited

Prints the reference information, by default to libMesh::out.

Definition at line 88 of file reference_counter.C.

References libMesh::ReferenceCounter::_enable_print_counter, and libMesh::ReferenceCounter::get_info().

Referenced by libMesh::LibMeshInit::LibMeshInit().

89 {
91  out_stream << ReferenceCounter::get_info();
92 }
static std::string get_info()
void libMesh::UnsteadySolver::reinit ( )
virtualinherited

The reinitialization function. This method is used to resize internal data vectors after a mesh change.

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::SecondOrderUnsteadySolver, and libMesh::AdaptiveTimeSolver.

Definition at line 70 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::GHOSTED, libMesh::NumericVector< T >::localize(), libMesh::System::n_dofs(), libMesh::System::n_local_dofs(), libMesh::UnsteadySolver::old_local_nonlinear_solution, libMesh::TimeSolver::reinit(), and libMesh::SERIAL.

Referenced by libMesh::SecondOrderUnsteadySolver::reinit().

71 {
73 
74 #ifdef LIBMESH_ENABLE_GHOSTED
77  GHOSTED);
78 #else
80 #endif
81 
82  // localize the old solution
83  NumericVector<Number> & old_nonlinear_soln =
84  _system.get_vector("_old_nonlinear_solution");
85 
86  old_nonlinear_soln.localize
89 }
virtual void reinit()
Definition: time_solver.C:48
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
const NumericVector< Number > & get_vector(const std::string &vec_name) const
Definition: system.C:792
dof_id_type n_local_dofs() const
Definition: system.C:183
dof_id_type n_dofs() const
Definition: system.C:146
const std::vector< dof_id_type > & get_send_list() const
Definition: dof_map.h:394
virtual void localize(std::vector< T > &v_local) const =0
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
void libMesh::UnsteadySolver::retrieve_timestep ( )
virtualinherited

This method retrieves all the stored solutions at the current system.time

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::SecondOrderUnsteadySolver.

Definition at line 204 of file unsteady_solver.C.

References libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::NumericVector< T >::localize(), libMesh::UnsteadySolver::old_local_nonlinear_solution, and libMesh::TimeSolver::solution_history.

205 {
206  // Retrieve all the stored vectors at the current time
207  solution_history->retrieve();
208 
209  // Dont forget to localize the old_nonlinear_solution !
210  _system.get_vector("_old_nonlinear_solution").localize
213 }
sys_type & _system
Definition: time_solver.h:257
const DofMap & get_dof_map() const
Definition: system.h:2028
const NumericVector< Number > & get_vector(const std::string &vec_name) const
Definition: system.C:792
UniquePtr< SolutionHistory > solution_history
Definition: time_solver.h:264
const std::vector< dof_id_type > & get_send_list() const
Definition: dof_map.h:394
virtual void localize(std::vector< T > &v_local) const =0
UniquePtr< NumericVector< Number > > old_local_nonlinear_solution
void libMesh::TimeSolver::set_is_adjoint ( bool  _is_adjoint_value)
inlineinherited

Accessor for setting whether we need to do a primal or adjoint solve

Definition at line 239 of file time_solver.h.

References libMesh::TimeSolver::_is_adjoint.

Referenced by libMesh::DifferentiableSystem::adjoint_solve(), libMesh::FEMSystem::postprocess(), and libMesh::DifferentiableSystem::solve().

240  { _is_adjoint = _is_adjoint_value; }
void libMesh::TimeSolver::set_solution_history ( const SolutionHistory _solution_history)
inherited

A setter function users will employ if they need to do something other than save no solution history

Definition at line 97 of file time_solver.C.

References libMesh::SolutionHistory::clone(), and libMesh::TimeSolver::solution_history.

98 {
99  solution_history = _solution_history.clone();
100 }
UniquePtr< SolutionHistory > solution_history
Definition: time_solver.h:264
bool libMesh::Euler2Solver::side_residual ( bool  request_jacobian,
DiffContext context 
)
virtual

This method uses the DifferentiablePhysics' side_time_derivative() and side_constraint() to build a full residual on an element's side. What combination it uses will depend on theta.

Implements libMesh::TimeSolver.

Definition at line 67 of file euler2_solver.C.

References _general_residual(), libMesh::DiffContext::elem_side_reinit(), libMesh::DifferentiablePhysics::side_constraint(), libMesh::DifferentiablePhysics::side_damping_residual(), libMesh::DifferentiablePhysics::side_mass_residual(), and libMesh::DifferentiablePhysics::side_time_derivative().

69 {
70  return this->_general_residual(request_jacobian,
71  context,
77  false);
78 }
virtual bool side_constraint(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:190
virtual bool _general_residual(bool request_jacobian, DiffContext &, ResFuncType mass, ResFuncType damping, ResFuncType time_deriv, ResFuncType constraint, ReinitFuncType reinit, bool compute_second_order_eqns)
Definition: euler2_solver.C:99
virtual bool side_damping_residual(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:388
virtual void elem_side_reinit(Real)
Definition: diff_context.h:81
virtual bool side_mass_residual(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:332
virtual bool side_time_derivative(bool request_jacobian, DiffContext &)
Definition: diff_physics.h:170
void libMesh::UnsteadySolver::solve ( )
virtualinherited

This method solves for the solution at the next timestep. Usually we will only need to solve one (non)linear system per timestep, but more complex subclasses may override this.

Reimplemented from libMesh::TimeSolver.

Reimplemented in libMesh::NewmarkSolver, libMesh::AdaptiveTimeSolver, and libMesh::TwostepTimeSolver.

Definition at line 93 of file unsteady_solver.C.

References libMesh::TimeSolver::_diff_solver, libMesh::TimeSolver::_system, libMesh::UnsteadySolver::advance_timestep(), libMesh::DifferentiableSystem::deltat, libMesh::DiffSolver::DIVERGED_BACKTRACKING_FAILURE, libMesh::DiffSolver::DIVERGED_MAX_NONLINEAR_ITERATIONS, libMesh::UnsteadySolver::first_solve, libMesh::out, libMesh::TimeSolver::quiet, and libMesh::TimeSolver::reduce_deltat_on_diffsolver_failure.

Referenced by libMesh::NewmarkSolver::solve().

94 {
95  if (first_solve)
96  {
98  first_solve = false;
99  }
100 
101  unsigned int solve_result = _diff_solver->solve();
102 
103  // If we requested the UnsteadySolver to attempt reducing dt after a
104  // failed DiffSolver solve, check the results of the solve now.
106  {
107  bool backtracking_failed =
109 
110  bool max_iterations =
112 
113  if (backtracking_failed || max_iterations)
114  {
115  // Cut timestep in half
116  for (unsigned int nr=0; nr<reduce_deltat_on_diffsolver_failure; ++nr)
117  {
118  _system.deltat *= 0.5;
119  libMesh::out << "Newton backtracking failed. Trying with smaller timestep, dt="
120  << _system.deltat << std::endl;
121 
122  solve_result = _diff_solver->solve();
123 
124  // Check solve results with reduced timestep
125  bool backtracking_still_failed =
127 
128  bool backtracking_max_iterations =
130 
131  if (!backtracking_still_failed && !backtracking_max_iterations)
132  {
133  if (!quiet)
134  libMesh::out << "Reduced dt solve succeeded." << std::endl;
135  return;
136  }
137  }
138 
139  // If we made it here, we still couldn't converge the solve after
140  // reducing deltat
141  libMesh::out << "DiffSolver::solve() did not succeed after "
142  << reduce_deltat_on_diffsolver_failure
143  << " attempts." << std::endl;
144  libmesh_convergence_failure();
145 
146  } // end if (backtracking_failed || max_iterations)
147  } // end if (reduce_deltat_on_diffsolver_failure)
148 }
virtual void advance_timestep() libmesh_override
sys_type & _system
Definition: time_solver.h:257
unsigned int reduce_deltat_on_diffsolver_failure
Definition: time_solver.h:220
UniquePtr< DiffSolver > _diff_solver
Definition: time_solver.h:247
OStreamProxy out(std::cout)
const sys_type& libMesh::TimeSolver::system ( ) const
inlineinherited
Returns
A constant reference to the system we are solving.

Definition at line 171 of file time_solver.h.

References libMesh::TimeSolver::_system.

Referenced by libMesh::TimeSolver::reinit(), and libMesh::TimeSolver::solve().

171 { return _system; }
sys_type & _system
Definition: time_solver.h:257
sys_type& libMesh::TimeSolver::system ( )
inlineinherited
Returns
A writable reference to the system we are solving.

Definition at line 176 of file time_solver.h.

References libMesh::TimeSolver::_system.

176 { return _system; }
sys_type & _system
Definition: time_solver.h:257
virtual unsigned int libMesh::FirstOrderUnsteadySolver::time_order ( ) const
inlinevirtualinherited
Returns
The maximum order of time derivatives for which the UnsteadySolver subclass is capable of handling.

For example, EulerSolver will have time_order() = 1 and NewmarkSolver will have time_order() = 2.

Implements libMesh::UnsteadySolver.

Definition at line 90 of file first_order_unsteady_solver.h.

References libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), and libMesh::FirstOrderUnsteadySolver::prepare_accel().

91  { return 1; }

Member Data Documentation

ReferenceCounter::Counts libMesh::ReferenceCounter::_counts
staticprotectedinherited
UniquePtr<DiffSolver> libMesh::TimeSolver::_diff_solver
protectedinherited

An implicit linear or nonlinear solver to use at each timestep.

Definition at line 247 of file time_solver.h.

Referenced by libMesh::NewmarkSolver::compute_initial_accel(), libMesh::TimeSolver::diff_solver(), and libMesh::UnsteadySolver::solve().

bool libMesh::ReferenceCounter::_enable_print_counter = true
staticprotectedinherited

Flag to control whether reference count information is printed when print_info is called.

Definition at line 143 of file reference_counter.h.

Referenced by libMesh::ReferenceCounter::disable_print_counter_info(), libMesh::ReferenceCounter::enable_print_counter_info(), and libMesh::ReferenceCounter::print_info().

UniquePtr<LinearSolver<Number> > libMesh::TimeSolver::_linear_solver
protectedinherited

An implicit linear solver to use for adjoint problems.

Definition at line 252 of file time_solver.h.

Referenced by libMesh::TimeSolver::linear_solver().

Threads::spin_mutex libMesh::ReferenceCounter::_mutex
staticprotectedinherited

Mutual exclusion object to enable thread-safe reference counting.

Definition at line 137 of file reference_counter.h.

Threads::atomic< unsigned int > libMesh::ReferenceCounter::_n_objects
staticprotectedinherited

The number of objects. Print the reference count information when the number returns to 0.

Definition at line 132 of file reference_counter.h.

Referenced by libMesh::ReferenceCounter::n_objects(), libMesh::ReferenceCounter::ReferenceCounter(), and libMesh::ReferenceCounter::~ReferenceCounter().

sys_type& libMesh::TimeSolver::_system
protectedinherited

A reference to the system we are solving.

Definition at line 257 of file time_solver.h.

Referenced by libMesh::EulerSolver::_general_residual(), _general_residual(), libMesh::SteadySolver::_general_residual(), libMesh::NewmarkSolver::_general_residual(), libMesh::UnsteadySolver::adjoint_advance_timestep(), libMesh::NewmarkSolver::advance_timestep(), libMesh::AdaptiveTimeSolver::advance_timestep(), libMesh::UnsteadySolver::advance_timestep(), libMesh::NewmarkSolver::compute_initial_accel(), libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), libMesh::UnsteadySolver::du(), libMesh::EulerSolver::element_residual(), element_residual(), libMesh::EigenTimeSolver::element_residual(), libMesh::SecondOrderUnsteadySolver::init(), libMesh::UnsteadySolver::init(), libMesh::TimeSolver::init(), libMesh::EigenTimeSolver::init(), libMesh::SecondOrderUnsteadySolver::init_data(), libMesh::UnsteadySolver::init_data(), libMesh::TimeSolver::init_data(), libMesh::EulerSolver::nonlocal_residual(), nonlocal_residual(), libMesh::EigenTimeSolver::nonlocal_residual(), libMesh::UnsteadySolver::old_nonlinear_solution(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), libMesh::NewmarkSolver::project_initial_accel(), libMesh::SecondOrderUnsteadySolver::project_initial_rate(), libMesh::SecondOrderUnsteadySolver::reinit(), libMesh::UnsteadySolver::reinit(), libMesh::TimeSolver::reinit(), libMesh::UnsteadySolver::retrieve_timestep(), libMesh::EigenTimeSolver::side_residual(), libMesh::TwostepTimeSolver::solve(), libMesh::UnsteadySolver::solve(), libMesh::EigenTimeSolver::solve(), and libMesh::TimeSolver::system().

bool libMesh::UnsteadySolver::first_adjoint_step
protectedinherited

A bool that will be true the first time adjoint_advance_timestep() is called, (when the primal solution is to be used to set adjoint boundary conditions) and false thereafter

Definition at line 167 of file unsteady_solver.h.

Referenced by libMesh::UnsteadySolver::adjoint_advance_timestep().

bool libMesh::UnsteadySolver::first_solve
protectedinherited
bool libMesh::TimeSolver::quiet
inherited

Print extra debugging information if quiet == false.

Definition at line 191 of file time_solver.h.

Referenced by libMesh::TwostepTimeSolver::solve(), libMesh::UnsteadySolver::solve(), and libMesh::EigenTimeSolver::solve().

unsigned int libMesh::TimeSolver::reduce_deltat_on_diffsolver_failure
inherited

This value (which defaults to zero) is the number of times the TimeSolver is allowed to halve deltat and let the DiffSolver repeat the latest failed solve with a reduced timestep.

Note
This has no effect for SteadySolvers.
You must set at least one of the DiffSolver flags "continue_after_max_iterations" or "continue_after_backtrack_failure" to allow the TimeSolver to retry the solve.

Definition at line 220 of file time_solver.h.

Referenced by libMesh::TwostepTimeSolver::solve(), and libMesh::UnsteadySolver::solve().

UniquePtr<SolutionHistory> libMesh::TimeSolver::solution_history
protectedinherited

A UniquePtr to a SolutionHistory object. Default is NoSolutionHistory, which the user can override by declaring a different kind of SolutionHistory in the application

Definition at line 264 of file time_solver.h.

Referenced by libMesh::UnsteadySolver::adjoint_advance_timestep(), libMesh::UnsteadySolver::advance_timestep(), libMesh::UnsteadySolver::retrieve_timestep(), and libMesh::TimeSolver::set_solution_history().

Real libMesh::Euler2Solver::theta

The value for the theta method to employ: 1.0 corresponds to backwards Euler, 0.0 corresponds to forwards Euler, 0.5 corresponds to a Crank-Nicolson-like scheme.

Definition at line 105 of file euler2_solver.h.

Referenced by _general_residual(), and error_order().


The documentation for this class was generated from the following files: