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-/*
- * ***** BEGIN GPL LICENSE BLOCK *****
- *
- * This program is free software; you can redistribute it and/or
- * modify it under the terms of the GNU General Public License
- * as published by the Free Software Foundation; either version 2
- * of the License, or (at your option) any later version.
- *
- * This program is distributed in the hope that it will be useful,
- * but WITHOUT ANY WARRANTY; without even the implied warranty of
- * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
- * GNU General Public License for more details.
- *
- * You should have received a copy of the GNU General Public License
- * along with this program; if not, write to the Free Software Foundation,
- * Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301, USA.
- *
- * The Original Code is Copyright (C) 2001-2002 by NaN Holding BV.
- * All rights reserved.
- *
- * The Original Code is: all of this file.
- *
- * Original author: Laurence
- * Contributor(s): Brecht
- *
- * ***** END GPL LICENSE BLOCK *****
- */
-
-/** \file iksolver/intern/MT_ExpMap.h
- * \ingroup iksolver
- */
-
-
-#ifndef MT_ExpMap_H
-#define MT_ExpMap_H
-
-#include <MT_assert.h>
-
-#include "MT_Vector3.h"
-#include "MT_Quaternion.h"
-#include "MT_Matrix4x4.h"
-
-const MT_Scalar MT_EXPMAP_MINANGLE (1e-7);
-
-/**
- * MT_ExpMap an exponential map parameterization of rotations
- * in 3D. This implementation is derived from the paper
- * "F. Sebastian Grassia. Practical parameterization of
- * rotations using the exponential map. Journal of Graphics Tools,
- * 3(3):29-48, 1998" Please go to http://www.acm.org/jgt/papers/Grassia98/
- * for a thorough description of the theory and sample code used
- * to derive this class.
- *
- * Basic overview of why this class is used.
- * In an IK system we need to paramterize the joint angles in some
- * way. Typically 2 parameterizations are used.
- * - Euler Angles
- * These suffer from singularities in the parameterization known
- * as gimbal lock. They also do not interpolate well. For every
- * set of euler angles there is exactly 1 corresponding 3d rotation.
- * - Quaternions.
- * Great for interpolating. Only unit quaternions are valid rotations
- * means that in a differential ik solver we often stray outside of
- * this manifold into invalid rotations. Means we have to do a lot
- * of nasty normalizations all the time. Does not suffer from
- * gimbal lock problems. More expensive to compute partial derivatives
- * as there are 4 of them.
- *
- * So exponential map is similar to a quaternion axis/angle
- * representation but we store the angle as the length of the
- * axis. So require only 3 parameters. Means that all exponential
- * maps are valid rotations. Suffers from gimbal lock. But it's
- * possible to detect when gimbal lock is near and reparameterize
- * away from it. Also nice for interpolating.
- * Exponential maps are share some of the useful properties of
- * euler and quaternion parameterizations. And are very useful
- * for differential IK solvers.
- */
-
-class MT_ExpMap {
-public:
-
- /**
- * Default constructor
- * @warning there is no initialization in the
- * default constructor
- */
-
- MT_ExpMap() {}
- MT_ExpMap(const MT_Vector3& v) : m_v(v) { angleUpdated(); }
-
- MT_ExpMap(const float v[3]) : m_v(v) { angleUpdated(); }
- MT_ExpMap(const double v[3]) : m_v(v) { angleUpdated(); }
-
- MT_ExpMap(MT_Scalar x, MT_Scalar y, MT_Scalar z) :
- m_v(x, y, z) { angleUpdated(); }
-
- /**
- * Construct an exponential map from a quaternion
- */
-
- MT_ExpMap(
- const MT_Quaternion &q
- ) {
- setRotation(q);
- }
-
- /**
- * Accessors
- * Decided not to inherit from MT_Vector3 but rather
- * this class contains an MT_Vector3. This is because
- * it is very dangerous to use MT_Vector3 functions
- * on this class and some of them have no direct meaning.
- */
-
- const
- MT_Vector3 &
- vector(
- ) const {
- return m_v;
- }
-
- /**
- * Set the exponential map from a quaternion
- */
-
- void
- setRotation(
- const MT_Quaternion &q
- );
-
- /**
- * Convert from an exponential map to a quaternion
- * representation
- */
-
- const MT_Quaternion&
- getRotation(
- ) const;
-
- /**
- * Convert the exponential map to a 3x3 matrix
- */
-
- MT_Matrix3x3
- getMatrix(
- ) const;
-
- /**
- * Update (and reparameterize) the expontial map
- * @param dv delta update values.
- */
-
- void
- update(
- const MT_Vector3& dv
- );
-
- /**
- * Compute the partial derivatives of the exponential
- * map (dR/de - where R is a 4x4 matrix formed
- * from the map) and return them as a 4x4 matrix
- */
-
- void
- partialDerivatives(
- MT_Matrix3x3& dRdx,
- MT_Matrix3x3& dRdy,
- MT_Matrix3x3& dRdz
- ) const ;
-
-private :
-
- // m_v contains the exponential map, the other variables are
- // cached for efficiency
-
- MT_Vector3 m_v;
- MT_Scalar m_theta, m_sinp;
- MT_Quaternion m_q;
-
- // private methods
-
- // Compute partial derivatives dR (3x3 rotation matrix) / dVi (EM vector)
- // given the partial derivative dQ (Quaternion) / dVi (ith element of EM vector)
-
- void
- compute_dRdVi(
- const MT_Quaternion &dQdV,
- MT_Matrix3x3 & dRdVi
- ) const;
-
- // compute partial derivatives dQ/dVi
-
- void
- compute_dQdVi(
- MT_Quaternion *dQdX
- ) const ;
-
- // reparametrize away from singularity
-
- void
- reParametrize(
- );
-
- // (re-)compute cached variables
-
- void
- angleUpdated(
- );
-};
-
-#endif
-