MFEM
v4.1.0
Finite element discretization library
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#include <ode.hpp>
Public Member Functions | |
NewmarkSolver (double beta_=0.25, double gamma_=0.5) | |
virtual void | PrintProperties (std::ostream &out=mfem::out) |
virtual void | Init (SecondOrderTimeDependentOperator &_f) |
Associate a TimeDependentOperator with the ODE solver. More... | |
virtual void | Step (Vector &x, Vector &dxdt, double &t, double &dt) |
Perform a time step from time t [in] to time t [out] based on the requested step size dt [in]. More... | |
Public Member Functions inherited from mfem::SecondOrderODESolver | |
SecondOrderODESolver () | |
virtual void | Run (Vector &x, Vector &dxdt, double &t, double &dt, double tf) |
Perform time integration from time t [in] to time tf [in]. More... | |
virtual | ~SecondOrderODESolver () |
Additional Inherited Members | |
Protected Attributes inherited from mfem::SecondOrderODESolver | |
SecondOrderTimeDependentOperator * | f |
Pointer to the associated TimeDependentOperator. More... | |
MemoryType | mem_type |
The classical newmark method. Newmark, N. M. (1959) A method of computation for structural dynamics. Journal of Engineering Mechanics, ASCE, 85 (EM3) 67-94.
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inline |
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virtual |
Associate a TimeDependentOperator with the ODE solver.
This method has to be called:
Reimplemented from mfem::SecondOrderODESolver.
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virtual |
Perform a time step from time t [in] to time t [out] based on the requested step size dt [in].
[in,out] | x | Approximate solution. |
[in,out] | dxdt | Approximate rate. |
[in,out] | t | Time associated with the approximate solution x and rate @ dxdt |
[in,out] | dt | Time step size. |
The following rules describe the common behavior of the method:
Implements mfem::SecondOrderODESolver.