Symplectic 2nd-order explicit time-integrator for rigid-body motion. More...

Inheritance diagram for symplectic:

Collaboration diagram for symplectic:

Public Member Functions
	TypeName ("symplectic")
	Runtime type information. More...

	symplectic (rigidBodyMotion &body, const dictionary &dict)
	Construct for the given body from dictionary. More...

virtual	~symplectic ()
	Destructor. More...

virtual void	solve (const scalarField &tau, const Field< spatialVector > &fx)
	Integrate the rigid-body motion for one time-step. More...

Public Member Functions inherited from rigidBodySolver
	TypeName ("rigidBodySolver")
	Runtime type information. More...

	declareRunTimeSelectionTable (autoPtr, rigidBodySolver, dictionary,(rigidBodyMotion &body, const dictionary &dict),(body, dict))

	rigidBodySolver (rigidBodyMotion &body)

virtual	~rigidBodySolver ()
	Destructor. More...

Additional Inherited Members
Static Public Member Functions inherited from rigidBodySolver
static autoPtr< rigidBodySolver >	New (rigidBodyMotion &body, const dictionary &dict)

Protected Member Functions inherited from rigidBodySolver
rigidBodyModelState &	state ()
	Return the motion state. More...

scalarField &	q ()
	Return the current joint position and orientation. More...

scalarField &	qDot ()
	Return the current joint quaternion. More...

scalarField &	qDdot ()
	Return the current joint acceleration. More...

scalar	deltaT () const
	Return the current time-step. More...

const rigidBodyModelState &	state0 () const
	Return the previous motion state. More...

const scalarField &	q0 () const
	Return the current joint position and orientation. More...

const scalarField &	qDot0 () const
	Return the current joint quaternion. More...

const scalarField &	qDdot0 () const
	Return the current joint acceleration. More...

scalar	deltaT0 () const
	Return the previous time-step. More...

void	correctQuaternionJoints ()
	Correct the quaternion joints based on the current change in q. More...

Protected Attributes inherited from rigidBodySolver
rigidBodyMotion &	model_
	The rigid-body model. More...

Detailed Description

Symplectic 2nd-order explicit time-integrator for rigid-body motion.

Reference:

    Dullweber, A., Leimkuhler, B., & McLachlan, R. (1997).
    Symplectic splitting methods for rigid body molecular dynamics.
    The Journal of chemical physics, 107(15), 5840-5851.

Can only be used for explicit integration of the motion of the body, i.e. may only be called once per time-step, no outer-correctors may be applied. For implicit integration with outer-correctors choose either CrankNicolson or Newmark schemes.

Example specification in dynamicMeshDict:

solver
{
    type    symplectic;
}

See also: Foam::RBD::rigidBodySolvers::CrankNicolson Foam::RBD::rigidBodySolvers::Newmark

Source files

Definition at line 76 of file symplectic.H.

Constructor & Destructor Documentation

◆ symplectic()

symplectic	(	rigidBodyMotion &	body,
		const dictionary &	dict
	)

Construct for the given body from dictionary.

Definition at line 47 of file symplectic.C.

◆ ~symplectic()

~symplectic ( )

virtual

Destructor.

Definition at line 58 of file symplectic.C.

References symplectic::solve().

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Member Function Documentation

◆ TypeName()

TypeName ( "symplectic" )

Runtime type information.

◆ solve()

void solve	(	const scalarField &	tau,
		const Field< spatialVector > &	fx
	)

virtual

Integrate the rigid-body motion for one time-step.

Implements rigidBodySolver.

Definition at line 65 of file symplectic.C.

Referenced by symplectic::~symplectic().

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

src/rigidBodyDynamics/rigidBodySolvers/symplectic/symplectic.H
src/rigidBodyDynamics/rigidBodySolvers/symplectic/symplectic.C

Public Member Functions