#include <CRBAlgorithm.h>
Inheritance diagram for Physsim::CRBAlgorithm:

Public Member Functions | |
| virtual void | clone (BasePtr &cloned, bimap< BasePtr, BasePtr > *obj_map=NULL) const |
| Implements Base::clone(). | |
| virtual void | load_state (BaseConstPtr object, bimap< BasePtr, BasePtr > *correspondence=NULL) |
| Implements Base::load_state(). | |
| virtual void | save_state (BasePtr object, bimap< BasePtr, BasePtr > *correspondence=NULL) const |
| Implements Base::save_state(). | |
| virtual void | calc_fwd_dyn (RCArticulatedBodyPtr body, ReferenceFrameType rftype) |
| Executes the composite rigid-body method. | |
| virtual void | apply_impulse (RCArticulatedBodyPtr body, const Vector3 &j, const Vector3 &k, const Vector3 &contact_point, RigidBodyPtr link) |
| Implements RCArticulatedBodyFwdDynAlgo::apply_impulse(). | |
| virtual void | load_from_xml (XMLTreeConstPtr node, std::map< std::string, BasePtr > &id_map) |
| Implements Base::load_from_xml(). | |
| virtual void | save_to_xml (XMLTreePtr node, std::list< BaseConstPtr > &shared_objects) const |
| Implements Base::save_to_xml(). | |
Public Attributes | |
| std::vector< SVector6 > | _v |
| The vector of spatial velocities determined in last call to calc_fwd_dyn(). | |
| SVector6 | _a0 |
| The spatial acceleration of the base computed on the last call to calc_fwd_dyn(). | |
| VectorN | _qdd |
| The vector of joint accelerations computed on the last call to calc_fwd_dyn(). | |
| std::vector< SMatrix6 > | _Iiso |
| The spatial isolated inertias. | |
| SMatrix6 | _Ic0 |
| The composite spatial inertia matrix for the base (only for floating bases) computed on the last call to calc_fwd_dyn(). | |
| SVector6 | _f0 |
| The spatial vector of forces on the base (only for floating-bases) computed on the last call to calc_fwd_dyn(). | |
| SMatrixN | _K |
| The matrix "K" as described by Featherstone on p. 123 computed in the last call to calc_fwd_dyn(). | |
| MatrixNN | _inv_aug |
| The inverse of the augmented matrix [I_0^c K; K^s H] used to compute forward dynamics for floating bases (see [Featherstone 1987], p. 123); note that we compute this b/c we generally may need to solve multiple systems of linear equations using this matrix as a LHS at different times. | |
| MatrixNN | _H |
| The joint-space inertia matrix computed in the last call to calc_fwd_dyn(). | |
| MatrixNN | _inv_H |
| The inverse of H (note: we compute this b/c we generally may need to solve multiple systems of linear equations using H as a LHS at different times). | |
| VectorN | _Q |
| The vector of joint actuator forces used in the last call to calc_fwd_dyn(). | |
| VectorN | _C |
| The vector "C" (as called by Featherstone) used in the last call to calc_fwd_dyn(). | |
| void CRBAlgorithm::apply_impulse | ( | RCArticulatedBodyPtr | body, | |
| const Vector3 & | jj, | |||
| const Vector3 & | jk, | |||
| const Vector3 & | point, | |||
| RigidBodyPtr | link | |||
| ) | [virtual] |
Implements RCArticulatedBodyFwdDynAlgo::apply_impulse().
Implements Physsim::RCArticulatedBodyFwdDynAlgo.
The vector "C" (as called by Featherstone) used in the last call to calc_fwd_dyn().
This vector is a sum of the Coriolis, centrifugal, and other forces on the body (all forces except actuator forces).
1.5.1