libMesh::NewmarkSolver Class Reference

This class defines a Newmark time integrator for second order (in time) DifferentiableSystems. More...

#include <newmark_solver.h>

Inheritance diagram for libMesh::NewmarkSolver:

Public Types
typedef UnsteadySolver	Parent
	The parent class. More...
typedef DifferentiableSystem	sys_type
	The type of system. More...

Public Member Functions
	NewmarkSolver (sys_type &s)
	Constructor. More...
virtual	~NewmarkSolver ()
	Destructor. More...
virtual void	advance_timestep () override
	This method advances the solution to the next timestep, after a solve() has been performed. More...
virtual void	adjoint_advance_timestep () override
	This method advances the adjoint solution to the previous timestep, after an adjoint_solve() has been performed. More...
virtual void	compute_initial_accel ()
	This method uses the specified initial displacement and velocity to compute the initial acceleration \(a_0\). More...
void	project_initial_accel (FunctionBase< Number > *f, FunctionBase< Gradient > *g=nullptr)
	Specify non-zero initial acceleration. More...
void	set_initial_accel_avail (bool initial_accel_set)
	Allow the user to (re)set whether the initial acceleration is available. More...
virtual Real	error_order () const override
	Error convergence order: 2 for \(\gamma=0.5\), 1 otherwise. More...
virtual void	solve () override
	This method solves for the solution at the next timestep. More...
virtual bool	element_residual (bool request_jacobian, DiffContext &) override
	This method uses the DifferentiablePhysics' element_time_derivative() and element_constraint() to build a full residual on an element. More...
virtual bool	side_residual (bool request_jacobian, DiffContext &) override
	This method uses the DifferentiablePhysics' side_time_derivative() and side_constraint() to build a full residual on an element's side. More...
virtual bool	nonlocal_residual (bool request_jacobian, DiffContext &) override
	This method uses the DifferentiablePhysics' nonlocal_time_derivative() and nonlocal_constraint() to build a full residual for non-local terms. More...
void	set_beta (Real beta)
	Setter for \( \beta \). More...
void	set_gamma (Real gamma)
	Setter for \( \gamma \). More...
virtual unsigned int	time_order () const override
virtual void	init () override
	The initialization function. More...
virtual void	init_data () override
	The data initialization function. More...
virtual void	reinit () override
	The reinitialization function. More...
virtual void	retrieve_timestep () override
	This method retrieves all the stored solutions at the current system.time. More...
void	project_initial_rate (FunctionBase< Number > *f, FunctionBase< Gradient > *g=nullptr)
	Specify non-zero initial velocity. More...
Number	old_solution_rate (const dof_id_type global_dof_number) const
Number	old_solution_accel (const dof_id_type global_dof_number) const
Number	old_nonlinear_solution (const dof_id_type global_dof_number) const
virtual Real	du (const SystemNorm &norm) const override
	Computes the size of ||u^{n+1} - u^{n}|| in some norm. More...
virtual bool	is_steady () const override
	This is not a steady-state solver. More...
virtual void	before_timestep ()
	This method is for subclasses or users to override to do arbitrary processing between timesteps. More...
const sys_type &	system () const
sys_type &	system ()
virtual std::unique_ptr< DiffSolver > &	diff_solver ()
	An implicit linear or nonlinear solver to use at each timestep. More...
virtual std::unique_ptr< LinearSolver< Number > > &	linear_solver ()
	An implicit linear solver to use for adjoint and sensitivity problems. More...
void	set_solution_history (const SolutionHistory &_solution_history)
	A setter function users will employ if they need to do something other than save no solution history. More...
bool	is_adjoint () const
	Accessor for querying whether we need to do a primal or adjoint solve. More...
void	set_is_adjoint (bool _is_adjoint_value)
	Accessor for setting whether we need to do a primal or adjoint solve. More...

Static Public Member Functions
static std::string	get_info ()
	Gets a string containing the reference information. More...
static void	print_info (std::ostream &out=libMesh::out)
	Prints the reference information, by default to libMesh::out. More...
static unsigned int	n_objects ()
	Prints the number of outstanding (created, but not yet destroyed) objects. More...
static void	enable_print_counter_info ()
	Methods to enable/disable the reference counter output from print_info() More...
static void	disable_print_counter_info ()

Public Attributes
std::unique_ptr< NumericVector< Number > >	old_local_nonlinear_solution
	Serial vector of _system.get_vector("_old_nonlinear_solution") More...
bool	quiet
	Print extra debugging information if quiet == false. More...
unsigned int	reduce_deltat_on_diffsolver_failure
	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. More...

Protected Types
typedef bool(DifferentiablePhysics::*	ResFuncType) (bool, DiffContext &)
	Definitions of argument types for use in refactoring subclasses. More...
typedef void(DiffContext::*	ReinitFuncType) (Real)
typedef std::map< std::string, std::pair< unsigned int, unsigned int > >	Counts
	Data structure to log the information. More...

Protected Member Functions
virtual bool	_general_residual (bool request_jacobian, DiffContext &, ResFuncType mass, ResFuncType damping, ResFuncType time_deriv, ResFuncType constraint, ReinitFuncType reinit)
	This method is the underlying implementation of the public residual methods. More...
void	increment_constructor_count (const std::string &name)
	Increments the construction counter. More...
void	increment_destructor_count (const std::string &name)
	Increments the destruction counter. More...

Protected Attributes
Real	_beta
	The value for the \(\beta\) to employ. More...
Real	_gamma
	The value for \(\gamma\) to employ. More...
bool	_is_accel_solve
	Need to be able to indicate to _general_residual if we are doing an acceleration solve or not. More...
bool	_initial_accel_set
	This method requires an initial acceleration. More...
std::unique_ptr< NumericVector< Number > >	_old_local_solution_rate
	Serial vector of previous time step velocity \( \dot{u}_n \). More...
std::unique_ptr< NumericVector< Number > >	_old_local_solution_accel
	Serial vector of previous time step acceleration \( \ddot{u}_n \). More...
bool	first_solve
	A bool that will be true the first time solve() is called, and false thereafter. More...
bool	first_adjoint_step
	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. More...
std::unique_ptr< DiffSolver >	_diff_solver
	An implicit linear or nonlinear solver to use at each timestep. More...
std::unique_ptr< LinearSolver< Number > >	_linear_solver
	An implicit linear solver to use for adjoint problems. More...
sys_type &	_system
	A reference to the system we are solving. More...
std::unique_ptr< SolutionHistory >	solution_history
	A std::unique_ptr to a SolutionHistory object. More...

Static Protected Attributes
static Counts	_counts
	Actually holds the data. More...
static Threads::atomic< unsigned int >	_n_objects
	The number of objects. More...
static Threads::spin_mutex	_mutex
	Mutual exclusion object to enable thread-safe reference counting. More...
static bool	_enable_print_counter = true
	Flag to control whether reference count information is printed when print_info is called. More...

Private Attributes
bool	_is_adjoint
	This boolean tells the TimeSolver whether we are solving a primal or adjoint problem. More...

Detailed Description

This class defines a Newmark time integrator for second order (in time) DifferentiableSystems.

There are two parameters \(\gamma\) and \(\beta\) (defaulting to 0.5 and 0.25, respectively).

Note

Projectors are included for the initial velocity and acceleration; the initial displacement can be set by calling System::project_solution().

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

Paul T. Bauman

Date

2015

Definition at line 46 of file newmark_solver.h.

Member Typedef Documentation

Counts

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 117 of file reference_counter.h.

Parent

typedef UnsteadySolver libMesh::NewmarkSolver::Parent

The parent class.

Definition at line 52 of file newmark_solver.h.

ReinitFuncType

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

protectedinherited

Definition at line 272 of file time_solver.h.

ResFuncType

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.

sys_type

typedef DifferentiableSystem libMesh::TimeSolver::sys_type

inherited

The type of system.

Definition at line 64 of file time_solver.h.

Constructor & Destructor Documentation

NewmarkSolver()

libMesh::NewmarkSolver::NewmarkSolver ( sys_type &  s )

explicit

Constructor.

Requires a reference to the system to be solved.

Definition at line 25 of file newmark_solver.C.

  : SecondOrderUnsteadySolver(s),
    _beta(0.25),
    _gamma(0.5),
    _is_accel_solve(false),
    _initial_accel_set(false)
{}

~NewmarkSolver()

libMesh::NewmarkSolver::~NewmarkSolver ( )

virtual

Destructor.

Definition at line 33 of file newmark_solver.C.

{}

Member Function Documentation

_general_residual()

bool libMesh::NewmarkSolver::_general_residual ( bool  request_jacobian, DiffContext &  context, ResFuncType  mass, ResFuncType  damping, ResFuncType  time_deriv, ResFuncType  constraint, ReinitFuncType  reinit  )

protectedvirtual

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

Definition at line 205 of file newmark_solver.C.

{
  unsigned int n_dofs = context.get_elem_solution().size();
 
  // We might need to save the old jacobian in case one of our physics
  // terms later is unable to update it analytically.
  DenseMatrix<Number> old_elem_jacobian(n_dofs, n_dofs);
 
  // Local velocity at old time step
  DenseVector<Number> old_elem_solution_rate(n_dofs);
  for (unsigned int i=0; i != n_dofs; ++i)
    old_elem_solution_rate(i) =
      old_solution_rate(context.get_dof_indices()[i]);
 
  // The user is computing the initial acceleration
  // So upstream we've swapped _system.solution and _old_local_solution_accel
  // So we need to give the context the correct entries since we're solving for
  // acceleration here.
  if (_is_accel_solve)
    {
      // System._solution is actually the acceleration right now so we need
      // to reset the elem_solution to the right thing, which in this case
      // is the initial guess for displacement, which got swapped into
      // _old_solution_accel vector
      DenseVector<Number> old_elem_solution(n_dofs);
      for (unsigned int i=0; i != n_dofs; ++i)
        old_elem_solution(i) =
          old_solution_accel(context.get_dof_indices()[i]);
 
      context.elem_solution_derivative = 0.0;
      context.elem_solution_rate_derivative = 0.0;
      context.elem_solution_accel_derivative = 1.0;
 
      // Acceleration is currently the unknown so it's already sitting
      // in elem_solution() thanks to FEMContext::pre_fe_reinit
      context.get_elem_solution_accel() = context.get_elem_solution();
 
      // Now reset elem_solution() to what the user is expecting
      context.get_elem_solution() = old_elem_solution;
 
      context.get_elem_solution_rate() = old_elem_solution_rate;
 
      // The user's Jacobians will be targeting derivatives w.r.t. u_{n+1}.
      // Although the vast majority of cases will have the correct analytic
      // Jacobians in this iteration, since we reset elem_solution_derivative*,
      // if there are coupled/overlapping problems, there could be
      // mismatches in the Jacobian. So we force finite differencing for
      // the first iteration.
      request_jacobian = false;
    }
  // Otherwise, the unknowns are the displacements and everything is straight
  // forward and is what you think it is
  else
    {
      if (request_jacobian)
        old_elem_jacobian.swap(context.get_elem_jacobian());
 
      // Local displacement at old timestep
      DenseVector<Number> old_elem_solution(n_dofs);
      for (unsigned int i=0; i != n_dofs; ++i)
        old_elem_solution(i) =
          old_nonlinear_solution(context.get_dof_indices()[i]);
 
      // Local acceleration at old time step
      DenseVector<Number> old_elem_solution_accel(n_dofs);
      for (unsigned int i=0; i != n_dofs; ++i)
        old_elem_solution_accel(i) =
          old_solution_accel(context.get_dof_indices()[i]);
 
      // Convenience
      libMesh::Real dt = _system.deltat;
 
      context.elem_solution_derivative = 1.0;
 
      // Local velocity at current time step
      // v_{n+1} = gamma/(beta*Delta t)*(x_{n+1}-x_n)
      //         + (1-(gamma/beta))*v_n
      //         + (1-gamma/(2*beta))*(Delta t)*a_n
      context.elem_solution_rate_derivative = (_gamma/(_beta*dt));
 
      context.get_elem_solution_rate()  = context.get_elem_solution();
      context.get_elem_solution_rate() -= old_elem_solution;
      context.get_elem_solution_rate() *= context.elem_solution_rate_derivative;
      context.get_elem_solution_rate().add( (1.0-_gamma/_beta), old_elem_solution_rate);
      context.get_elem_solution_rate().add( (1.0-_gamma/(2.0*_beta))*dt, old_elem_solution_accel);
 
 
 
      // Local acceleration at current time step
      // a_{n+1} = (1/(beta*(Delta t)^2))*(x_{n+1}-x_n)
      //         - 1/(beta*Delta t)*v_n
      //         - (1/(2*beta)-1)*a_n
      context.elem_solution_accel_derivative = 1.0/(_beta*dt*dt);
 
      context.get_elem_solution_accel()  = context.get_elem_solution();
      context.get_elem_solution_accel() -= old_elem_solution;
      context.get_elem_solution_accel() *= context.elem_solution_accel_derivative;
      context.get_elem_solution_accel().add(-1.0/(_beta*dt), old_elem_solution_rate);
      context.get_elem_solution_accel().add(-(1.0/(2.0*_beta)-1.0), old_elem_solution_accel);
 
      // Move the mesh into place first if necessary, set t = t_{n+1}
      (context.*reinit_func)(1.);
    }
 
  // If a fixed solution is requested, we'll use x_{n+1}
  if (_system.use_fixed_solution)
    context.get_elem_fixed_solution() = context.get_elem_solution();
 
  // Get the time derivative at t_{n+1}, F(u_{n+1})
  bool jacobian_computed = (_system.get_physics()->*time_deriv)(request_jacobian, context);
 
  // Damping at t_{n+1}, C(u_{n+1})
  jacobian_computed = (_system.get_physics()->*damping)(jacobian_computed, context) &&
    jacobian_computed;
 
  // Mass at t_{n+1}, M(u_{n+1})
  jacobian_computed = (_system.get_physics()->*mass)(jacobian_computed, context) &&
    jacobian_computed;
 
  // Add the constraint term
  jacobian_computed = (_system.get_physics()->*constraint)(jacobian_computed, context) &&
    jacobian_computed;
 
  // Add back (or restore) the old jacobian
  if (request_jacobian)
    {
      if (jacobian_computed)
        context.get_elem_jacobian() += old_elem_jacobian;
      else
        context.get_elem_jacobian().swap(old_elem_jacobian);
    }
 
  return jacobian_computed;
}

References _beta, _gamma, _is_accel_solve, libMesh::TimeSolver::_system, libMesh::DenseVector< T >::add(), libMesh::DifferentiableSystem::deltat, libMesh::DiffContext::elem_solution_accel_derivative, libMesh::DiffContext::elem_solution_derivative, libMesh::DiffContext::elem_solution_rate_derivative, libMesh::DiffContext::get_dof_indices(), libMesh::DiffContext::get_elem_fixed_solution(), libMesh::DiffContext::get_elem_jacobian(), libMesh::DiffContext::get_elem_solution(), libMesh::DiffContext::get_elem_solution_accel(), libMesh::DiffContext::get_elem_solution_rate(), libMesh::DifferentiableSystem::get_physics(), libMesh::UnsteadySolver::old_nonlinear_solution(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), libMesh::Real, libMesh::DenseVector< T >::size(), libMesh::DenseMatrix< T >::swap(), and libMesh::System::use_fixed_solution.

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

adjoint_advance_timestep()

void libMesh::NewmarkSolver::adjoint_advance_timestep ( )

overridevirtual

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::UnsteadySolver.

Definition at line 101 of file newmark_solver.C.

{
  libmesh_not_implemented();
}

advance_timestep()

void libMesh::NewmarkSolver::advance_timestep ( )

overridevirtual

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::UnsteadySolver.

Definition at line 43 of file newmark_solver.C.

{
  // We need to update velocity and acceleration before
  // we update the nonlinear solution (displacement) and
  // delta_t
 
  NumericVector<Number> & old_solution_rate =
    _system.get_vector("_old_solution_rate");
 
  NumericVector<Number> & old_solution_accel =
    _system.get_vector("_old_solution_accel");
 
  if (!first_solve)
    {
      NumericVector<Number> & old_nonlinear_soln =
        _system.get_vector("_old_nonlinear_solution");
 
      NumericVector<Number> & nonlinear_solution =
        *(_system.solution);
 
      // We need to cache the new solution_rate before updating the old_solution_rate
      // so we can update acceleration with the proper old_solution_rate
      // v_{n+1} = gamma/(beta*Delta t)*(x_{n+1}-x_n)
      //         - ((gamma/beta)-1)*v_n
      //         - (gamma/(2*beta)-1)*(Delta t)*a_n
      std::unique_ptr<NumericVector<Number>> new_solution_rate = nonlinear_solution.clone();
      (*new_solution_rate) -= old_nonlinear_soln;
      (*new_solution_rate) *= (_gamma/(_beta*_system.deltat));
      new_solution_rate->add( (1.0-_gamma/_beta), old_solution_rate );
      new_solution_rate->add( (1.0-_gamma/(2.0*_beta))*_system.deltat, old_solution_accel );
 
      // a_{n+1} = (1/(beta*(Delta t)^2))*(x_{n+1}-x_n)
      //         - 1/(beta*Delta t)*v_n
      //         - (1-1/(2*beta))*a_n
      std::unique_ptr<NumericVector<Number>> new_solution_accel = old_solution_accel.clone();
      (*new_solution_accel) *=  -(1.0/(2.0*_beta)-1.0);
      new_solution_accel->add( -1.0/(_beta*_system.deltat), old_solution_rate );
      new_solution_accel->add( 1.0/(_beta*_system.deltat*_system.deltat), nonlinear_solution );
      new_solution_accel->add( -1.0/(_beta*_system.deltat*_system.deltat), old_nonlinear_soln );
 
      // Now update old_solution_rate
      old_solution_rate = (*new_solution_rate);
      old_solution_accel = (*new_solution_accel);
    }
 
  // Localize updated vectors
  old_solution_rate.localize
    (*_old_local_solution_rate,
     _system.get_dof_map().get_send_list());
 
  old_solution_accel.localize
    (*_old_local_solution_accel,
     _system.get_dof_map().get_send_list());
 
  // Now we can finish advancing the timestep
  UnsteadySolver::advance_timestep();
}

References _beta, _gamma, libMesh::SecondOrderUnsteadySolver::_old_local_solution_accel, libMesh::SecondOrderUnsteadySolver::_old_local_solution_rate, libMesh::TimeSolver::_system, libMesh::NumericVector< T >::add(), libMesh::UnsteadySolver::advance_timestep(), libMesh::NumericVector< T >::clone(), libMesh::DifferentiableSystem::deltat, libMesh::UnsteadySolver::first_solve, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), and libMesh::System::solution.

before_timestep()

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.

{}

compute_initial_accel()

void libMesh::NewmarkSolver::compute_initial_accel ( )

virtual

This method uses the specified initial displacement and velocity to compute the initial acceleration \(a_0\).

Definition at line 106 of file newmark_solver.C.

{
  // We need to compute the initial acceleration based off of
  // the initial position and velocity and, thus, acceleration
  // is the unknown in diff_solver and not the displacement. So,
  // We swap solution and acceleration. NewmarkSolver::_general_residual
  // will check _is_accel_solve and provide the correct
  // values to the FEMContext assuming this swap was made.
  this->_is_accel_solve = true;
 
  //solution->accel, accel->solution
  _system.solution->swap(_system.get_vector("_old_solution_accel"));
  _system.update();
 
  this->_diff_solver->solve();
 
  // solution->solution, accel->accel
  _system.solution->swap(_system.get_vector("_old_solution_accel"));
  _system.update();
 
  // We're done, so no longer doing an acceleration solve
  this->_is_accel_solve = false;
 
  this->set_initial_accel_avail(true);
}

References libMesh::TimeSolver::_diff_solver, _is_accel_solve, libMesh::TimeSolver::_system, libMesh::System::get_vector(), set_initial_accel_avail(), libMesh::System::solution, and libMesh::System::update().

Referenced by main().

diff_solver()

virtual std::unique_ptr<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.

{ return _diff_solver; }

References libMesh::TimeSolver::_diff_solver.

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

disable_print_counter_info()

void libMesh::ReferenceCounter::disable_print_counter_info ( )

staticinherited

Definition at line 106 of file reference_counter.C.

{
  _enable_print_counter = false;
  return;
}

References libMesh::ReferenceCounter::_enable_print_counter.

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

du()

Real libMesh::UnsteadySolver::du ( const SystemNorm &  norm ) const

overridevirtualinherited

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.

{
 
  std::unique_ptr<NumericVector<Number>> solution_copy =
    _system.solution->clone();
 
  solution_copy->add(-1., _system.get_vector("_old_nonlinear_solution"));
 
  solution_copy->close();
 
  return _system.calculate_norm(*solution_copy, norm);
}

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

element_residual()

bool libMesh::NewmarkSolver::element_residual ( bool  request_jacobian, DiffContext &  context  )

overridevirtual

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 163 of file newmark_solver.C.

{
  return this->_general_residual(request_jacobian,
                                 context,
                                 &DifferentiablePhysics::mass_residual,
                                 &DifferentiablePhysics::damping_residual,
                                 &DifferentiablePhysics::_eulerian_time_deriv,
                                 &DifferentiablePhysics::element_constraint,
                                 &DiffContext::elem_reinit);
}

References libMesh::DifferentiablePhysics::_eulerian_time_deriv(), _general_residual(), libMesh::DifferentiablePhysics::damping_residual(), libMesh::DiffContext::elem_reinit(), libMesh::DifferentiablePhysics::element_constraint(), and libMesh::DifferentiablePhysics::mass_residual().

enable_print_counter_info()

void libMesh::ReferenceCounter::enable_print_counter_info ( )

staticinherited

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

Definition at line 100 of file reference_counter.C.

{
  _enable_print_counter = true;
  return;
}

References libMesh::ReferenceCounter::_enable_print_counter.

error_order()

Real libMesh::NewmarkSolver::error_order ( ) const

overridevirtual

Error convergence order: 2 for \(\gamma=0.5\), 1 otherwise.

Implements libMesh::UnsteadySolver.

Definition at line 36 of file newmark_solver.C.

{
  if (_gamma == 0.5)
    return 2.;
  return 1.;
}

References _gamma.

get_info()

std::string libMesh::ReferenceCounter::get_info ( )

staticinherited

Gets a string containing the reference information.

Definition at line 47 of file reference_counter.C.

{
#if defined(LIBMESH_ENABLE_REFERENCE_COUNTING) && defined(DEBUG)
 
  std::ostringstream oss;
 
  oss << '\n'
      << " ---------------------------------------------------------------------------- \n"
      << "| Reference count information                                                |\n"
      << " ---------------------------------------------------------------------------- \n";
 
  for (const auto & pr : _counts)
    {
      const std::string name(pr.first);
      const unsigned int creations    = pr.second.first;
      const unsigned int destructions = pr.second.second;
 
      oss << "| " << name << " reference count information:\n"
          << "|  Creations:    " << creations    << '\n'
          << "|  Destructions: " << destructions << '\n';
    }
 
  oss << " ---------------------------------------------------------------------------- \n";
 
  return oss.str();
 
#else
 
  return "";
 
#endif
}

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

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

increment_constructor_count()

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 181 of file reference_counter.h.

{
  Threads::spin_mutex::scoped_lock lock(Threads::spin_mtx);
  std::pair<unsigned int, unsigned int> & p = _counts[name];
 
  p.first++;
}

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

Referenced by libMesh::ReferenceCountedObject< RBParametrized >::ReferenceCountedObject().

increment_destructor_count()

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 194 of file reference_counter.h.

{
  Threads::spin_mutex::scoped_lock lock(Threads::spin_mtx);
  std::pair<unsigned int, unsigned int> & p = _counts[name];
 
  p.second++;
}

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

Referenced by libMesh::ReferenceCountedObject< RBParametrized >::~ReferenceCountedObject().

init()

void libMesh::SecondOrderUnsteadySolver::init ( )

overridevirtualinherited

The initialization function.

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

Reimplemented from libMesh::UnsteadySolver.

Definition at line 34 of file second_order_unsteady_solver.C.

{
  UnsteadySolver::init();
 
  _system.add_vector("_old_solution_rate");
  _system.add_vector("_old_solution_accel");
}

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

init_data()

void libMesh::SecondOrderUnsteadySolver::init_data ( )

overridevirtualinherited

The data initialization function.

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

Reimplemented from libMesh::UnsteadySolver.

Definition at line 42 of file second_order_unsteady_solver.C.

{
  UnsteadySolver::init_data();
 
#ifdef LIBMESH_ENABLE_GHOSTED
  _old_local_solution_rate->init (_system.n_dofs(), _system.n_local_dofs(),
                                  _system.get_dof_map().get_send_list(), false,
                                  GHOSTED);
 
  _old_local_solution_accel->init (_system.n_dofs(), _system.n_local_dofs(),
                                   _system.get_dof_map().get_send_list(), false,
                                   GHOSTED);
#else
  _old_local_solution_rate->init (_system.n_dofs(), false, SERIAL);
  _old_local_solution_accel->init (_system.n_dofs(), false, SERIAL);
#endif
}

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

is_adjoint()

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.

  { return _is_adjoint; }

References libMesh::TimeSolver::_is_adjoint.

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

is_steady()

virtual bool libMesh::UnsteadySolver::is_steady ( ) const

inlineoverridevirtualinherited

This is not a steady-state solver.

Implements libMesh::TimeSolver.

Definition at line 153 of file unsteady_solver.h.

{ return false; }

linear_solver()

virtual std::unique_ptr<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.

{ return _linear_solver; }

References libMesh::TimeSolver::_linear_solver.

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

n_objects()

static unsigned int libMesh::ReferenceCounter::n_objects ( )

inlinestaticinherited

Prints the number of outstanding (created, but not yet destroyed) objects.

Definition at line 83 of file reference_counter.h.

  { return _n_objects; }

References libMesh::ReferenceCounter::_n_objects.

nonlocal_residual()

bool libMesh::NewmarkSolver::nonlocal_residual ( bool  request_jacobian, DiffContext &  context  )

overridevirtual

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 191 of file newmark_solver.C.

{
  return this->_general_residual(request_jacobian,
                                 context,
                                 &DifferentiablePhysics::nonlocal_mass_residual,
                                 &DifferentiablePhysics::nonlocal_damping_residual,
                                 &DifferentiablePhysics::nonlocal_time_derivative,
                                 &DifferentiablePhysics::nonlocal_constraint,
                                 &DiffContext::nonlocal_reinit);
}

References _general_residual(), libMesh::DifferentiablePhysics::nonlocal_constraint(), libMesh::DifferentiablePhysics::nonlocal_damping_residual(), libMesh::DifferentiablePhysics::nonlocal_mass_residual(), libMesh::DiffContext::nonlocal_reinit(), and libMesh::DifferentiablePhysics::nonlocal_time_derivative().

old_nonlinear_solution()

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.

{
  libmesh_assert_less (global_dof_number, _system.get_dof_map().n_dofs());
  libmesh_assert_less (global_dof_number, old_local_nonlinear_solution->size());
 
  return (*old_local_nonlinear_solution)(global_dof_number);
}

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(), libMesh::Euler2Solver::_general_residual(), _general_residual(), and libMesh::FEMPhysics::eulerian_residual().

old_solution_accel()

Number libMesh::SecondOrderUnsteadySolver::old_solution_accel ( const dof_id_type  global_dof_number ) const

inherited

Returns

The solution acceleration at the previous time step, \(\ddot{u}_n\), for the specified global DOF.

Definition at line 116 of file second_order_unsteady_solver.C.

{
  libmesh_assert_less (global_dof_number, _system.get_dof_map().n_dofs());
  libmesh_assert_less (global_dof_number, _old_local_solution_accel->size());
 
  return (*_old_local_solution_accel)(global_dof_number);
}

References libMesh::SecondOrderUnsteadySolver::_old_local_solution_accel, libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), and libMesh::DofMap::n_dofs().

Referenced by _general_residual(), advance_timestep(), project_initial_accel(), and libMesh::SecondOrderUnsteadySolver::reinit().

old_solution_rate()

Number libMesh::SecondOrderUnsteadySolver::old_solution_rate ( const dof_id_type  global_dof_number ) const

inherited

Returns

The solution rate at the previous time step, \(\dot{u}_n\), for the specified global DOF.

Definition at line 107 of file second_order_unsteady_solver.C.

{
  libmesh_assert_less (global_dof_number, _system.get_dof_map().n_dofs());
  libmesh_assert_less (global_dof_number, _old_local_solution_rate->size());
 
  return (*_old_local_solution_rate)(global_dof_number);
}

References libMesh::SecondOrderUnsteadySolver::_old_local_solution_rate, libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), and libMesh::DofMap::n_dofs().

Referenced by _general_residual(), advance_timestep(), libMesh::SecondOrderUnsteadySolver::project_initial_rate(), and libMesh::SecondOrderUnsteadySolver::reinit().

print_info()

void libMesh::ReferenceCounter::print_info ( std::ostream &  out = libMesh::out )

staticinherited

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

Definition at line 87 of file reference_counter.C.

{
  if (_enable_print_counter)
    out_stream << ReferenceCounter::get_info();
}

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

project_initial_accel()

void libMesh::NewmarkSolver::project_initial_accel	(	FunctionBase< Number > *	f,
		FunctionBase< Gradient > *	g = nullptr
	)

Specify non-zero initial acceleration.

Should be called before solve(). This is an alternative to compute_initial_acceleration() if the initial acceleration is actually known. The function value f and its gradient g are user-provided cloneable functors. A gradient g is only required/used for projecting onto finite element spaces with continuous derivatives.

Definition at line 132 of file newmark_solver.C.

{
  NumericVector<Number> & old_solution_accel =
    _system.get_vector("_old_solution_accel");
 
  _system.project_vector( old_solution_accel, f, g );
 
  this->set_initial_accel_avail(true);
}

References libMesh::TimeSolver::_system, libMesh::System::get_vector(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::System::project_vector(), and set_initial_accel_avail().

project_initial_rate()

void libMesh::SecondOrderUnsteadySolver::project_initial_rate ( FunctionBase< Number > *  f, FunctionBase< Gradient > *  g = nullptr  )

inherited

Specify non-zero initial velocity.

Should be called before solve(). The function value f and its gradient g are user-provided cloneable functors. A gradient g is only required/used for projecting onto finite element spaces with continuous derivatives.

Definition at line 98 of file second_order_unsteady_solver.C.

{
  NumericVector<Number> & old_solution_rate =
    _system.get_vector("_old_solution_rate");
 
  _system.project_vector( old_solution_rate, f, g );
}

References libMesh::TimeSolver::_system, libMesh::System::get_vector(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), and libMesh::System::project_vector().

reinit()

void libMesh::SecondOrderUnsteadySolver::reinit ( )

overridevirtualinherited

The reinitialization function.

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

Reimplemented from libMesh::UnsteadySolver.

Definition at line 60 of file second_order_unsteady_solver.C.

{
  UnsteadySolver::reinit();
 
#ifdef LIBMESH_ENABLE_GHOSTED
  _old_local_solution_rate->init (_system.n_dofs(), _system.n_local_dofs(),
                                  _system.get_dof_map().get_send_list(), false,
                                  GHOSTED);
 
  _old_local_solution_accel->init (_system.n_dofs(), _system.n_local_dofs(),
                                   _system.get_dof_map().get_send_list(), false,
                                   GHOSTED);
#else
  _old_local_solution_rate->init (_system.n_dofs(), false, SERIAL);
  _old_local_solution_accel->init (_system.n_dofs(), false, SERIAL);
#endif
 
  // localize the old solutions
  NumericVector<Number> & old_solution_rate =
    _system.get_vector("_old_solution_rate");
 
  NumericVector<Number> & old_solution_accel =
    _system.get_vector("_old_solution_accel");
 
  old_solution_rate.localize
    (*_old_local_solution_rate,
     _system.get_dof_map().get_send_list());
 
  old_solution_accel.localize
    (*_old_local_solution_accel,
     _system.get_dof_map().get_send_list());
}

References libMesh::SecondOrderUnsteadySolver::_old_local_solution_accel, libMesh::SecondOrderUnsteadySolver::_old_local_solution_rate, libMesh::TimeSolver::_system, libMesh::System::get_dof_map(), libMesh::DofMap::get_send_list(), libMesh::System::get_vector(), libMesh::GHOSTED, libMesh::System::n_dofs(), libMesh::System::n_local_dofs(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), libMesh::UnsteadySolver::reinit(), and libMesh::SERIAL.

retrieve_timestep()

void libMesh::SecondOrderUnsteadySolver::retrieve_timestep ( )

overridevirtualinherited

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

Reimplemented from libMesh::UnsteadySolver.

Definition at line 93 of file second_order_unsteady_solver.C.

{
  libmesh_not_implemented();
}

set_beta()

void libMesh::NewmarkSolver::set_beta ( Real  beta )

inline

Setter for \( \beta \).

Definition at line 149 of file newmark_solver.h.

  { _beta = beta; }

References _beta.

set_gamma()

void libMesh::NewmarkSolver::set_gamma ( Real  gamma )

inline

Setter for \( \gamma \).

Note

The method is second order only for \( \gamma = 1/2 \).

Definition at line 157 of file newmark_solver.h.

  { _gamma = gamma; }

References _gamma.

set_initial_accel_avail()

void libMesh::NewmarkSolver::set_initial_accel_avail

(

bool

initial_accel_set

)

Allow the user to (re)set whether the initial acceleration is available.

This is not needed if either compute_initial_accel() or project_initial_accel() are called. This is useful is the user is restarting a calculation and the acceleration is available from the restart.

Definition at line 143 of file newmark_solver.C.

{
  _initial_accel_set = initial_accel_set;
}

References _initial_accel_set.

Referenced by compute_initial_accel(), and project_initial_accel().

set_is_adjoint()

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.

  { _is_adjoint = _is_adjoint_value; }

References libMesh::TimeSolver::_is_adjoint.

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

set_solution_history()

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 96 of file time_solver.C.

{
  solution_history = _solution_history.clone();
}

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

side_residual()

bool libMesh::NewmarkSolver::side_residual ( bool  request_jacobian, DiffContext &  context  )

overridevirtual

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 177 of file newmark_solver.C.

{
  return this->_general_residual(request_jacobian,
                                 context,
                                 &DifferentiablePhysics::side_mass_residual,
                                 &DifferentiablePhysics::side_damping_residual,
                                 &DifferentiablePhysics::side_time_derivative,
                                 &DifferentiablePhysics::side_constraint,
                                 &DiffContext::elem_side_reinit);
}

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().

solve()

void libMesh::NewmarkSolver::solve ( )

overridevirtual

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::UnsteadySolver.

Definition at line 148 of file newmark_solver.C.

{
  // First, check that the initial accel was set one way or another
  if (!_initial_accel_set)
    {
      std::string error = "ERROR: Must first set initial acceleration using one of:\n";
      error += "NewmarkSolver::compute_initial_accel()\n";
      error += "NewmarkSolver::project_initial_accel()\n";
      libmesh_error_msg(error);
    }
 
  // That satisfied, now we can solve
  UnsteadySolver::solve();
}

References _initial_accel_set, and libMesh::UnsteadySolver::solve().

system() [1/2]

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.

{ return _system; }

References libMesh::TimeSolver::_system.

system() [2/2]

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.

{ return _system; }

References libMesh::TimeSolver::_system.

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

time_order()

virtual unsigned int libMesh::SecondOrderUnsteadySolver::time_order ( ) const

inlineoverridevirtualinherited

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 53 of file second_order_unsteady_solver.h.

  { return 2; }

Member Data Documentation

_beta

Real libMesh::NewmarkSolver::_beta

protected

The value for the \(\beta\) to employ.

Method is unconditionally stable for \( \beta \ge \frac{1}{4} \left( \gamma + \frac{1}{2}\right)^2 \)

Definition at line 167 of file newmark_solver.h.

Referenced by _general_residual(), advance_timestep(), and set_beta().

_counts

ReferenceCounter::Counts libMesh::ReferenceCounter::_counts

staticprotectedinherited

Actually holds the data.

Definition at line 122 of file reference_counter.h.

Referenced by libMesh::ReferenceCounter::get_info(), libMesh::ReferenceCounter::increment_constructor_count(), and libMesh::ReferenceCounter::increment_destructor_count().

_diff_solver

std::unique_ptr<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 compute_initial_accel(), libMesh::TimeSolver::diff_solver(), and libMesh::UnsteadySolver::solve().

_enable_print_counter

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 141 of file reference_counter.h.

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

_gamma

Real libMesh::NewmarkSolver::_gamma

protected

The value for \(\gamma\) to employ.

Newmark is 2nd order iff \(\gamma=0.5\).

Definition at line 173 of file newmark_solver.h.

Referenced by _general_residual(), advance_timestep(), error_order(), and set_gamma().

_initial_accel_set

bool libMesh::NewmarkSolver::_initial_accel_set

protected

This method requires an initial acceleration.

So, we force the user to call either compute_initial_accel or project_initial_accel to set the initial acceleration.

Definition at line 187 of file newmark_solver.h.

Referenced by set_initial_accel_avail(), and solve().

_is_accel_solve

bool libMesh::NewmarkSolver::_is_accel_solve

protected

Need to be able to indicate to _general_residual if we are doing an acceleration solve or not.

Definition at line 179 of file newmark_solver.h.

Referenced by _general_residual(), and compute_initial_accel().

_is_adjoint

bool libMesh::TimeSolver::_is_adjoint

privateinherited

This boolean tells the TimeSolver whether we are solving a primal or adjoint problem.

Definition at line 280 of file time_solver.h.

Referenced by libMesh::TimeSolver::is_adjoint(), and libMesh::TimeSolver::set_is_adjoint().

_linear_solver

std::unique_ptr<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().

_mutex

Threads::spin_mutex libMesh::ReferenceCounter::_mutex

staticprotectedinherited

Mutual exclusion object to enable thread-safe reference counting.

Definition at line 135 of file reference_counter.h.

_n_objects

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 130 of file reference_counter.h.

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

_old_local_solution_accel

std::unique_ptr<NumericVector<Number> > libMesh::SecondOrderUnsteadySolver::_old_local_solution_accel

protectedinherited

Serial vector of previous time step acceleration \( \ddot{u}_n \).

Definition at line 112 of file second_order_unsteady_solver.h.

Referenced by advance_timestep(), libMesh::SecondOrderUnsteadySolver::init_data(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), and libMesh::SecondOrderUnsteadySolver::reinit().

_old_local_solution_rate

std::unique_ptr<NumericVector<Number> > libMesh::SecondOrderUnsteadySolver::_old_local_solution_rate

protectedinherited

Serial vector of previous time step velocity \( \dot{u}_n \).

Definition at line 107 of file second_order_unsteady_solver.h.

Referenced by advance_timestep(), libMesh::SecondOrderUnsteadySolver::init_data(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), and libMesh::SecondOrderUnsteadySolver::reinit().

_system

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(), libMesh::Euler2Solver::_general_residual(), libMesh::SteadySolver::_general_residual(), _general_residual(), libMesh::UnsteadySolver::adjoint_advance_timestep(), advance_timestep(), libMesh::AdaptiveTimeSolver::advance_timestep(), libMesh::UnsteadySolver::advance_timestep(), compute_initial_accel(), libMesh::FirstOrderUnsteadySolver::compute_second_order_eqns(), libMesh::UnsteadySolver::du(), libMesh::EulerSolver::element_residual(), libMesh::Euler2Solver::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(), libMesh::Euler2Solver::nonlocal_residual(), libMesh::EigenTimeSolver::nonlocal_residual(), libMesh::UnsteadySolver::old_nonlinear_solution(), libMesh::SecondOrderUnsteadySolver::old_solution_accel(), libMesh::SecondOrderUnsteadySolver::old_solution_rate(), 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().

first_adjoint_step

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().

first_solve

bool libMesh::UnsteadySolver::first_solve

protectedinherited

A bool that will be true the first time solve() is called, and false thereafter.

Definition at line 161 of file unsteady_solver.h.

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

old_local_nonlinear_solution

std::unique_ptr<NumericVector<Number> > libMesh::UnsteadySolver::old_local_nonlinear_solution

inherited

Serial vector of _system.get_vector("_old_nonlinear_solution")

Definition at line 137 of file unsteady_solver.h.

Referenced by libMesh::AdaptiveTimeSolver::AdaptiveTimeSolver(), libMesh::UnsteadySolver::adjoint_advance_timestep(), libMesh::UnsteadySolver::advance_timestep(), libMesh::AdaptiveTimeSolver::init(), libMesh::UnsteadySolver::init_data(), libMesh::UnsteadySolver::old_nonlinear_solution(), libMesh::UnsteadySolver::reinit(), libMesh::UnsteadySolver::retrieve_timestep(), and libMesh::AdaptiveTimeSolver::~AdaptiveTimeSolver().

quiet

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().

reduce_deltat_on_diffsolver_failure

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().

solution_history

std::unique_ptr<SolutionHistory> libMesh::TimeSolver::solution_history

protectedinherited

A std::unique_ptr 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().

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

• include/solvers/newmark_solver.h
• src/solvers/newmark_solver.C