2001-12-01 06:22:24 +00:00
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#include "Math.hpp"
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#include "RigidBody.hpp"
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namespace yasim {
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RigidBody::RigidBody()
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{
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// Allocate space for 16 masses initially. More space will be
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// allocated dynamically.
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_nMasses = 0;
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_massesAlloced = 16;
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_masses = new Mass[_massesAlloced];
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_gyro[0] = _gyro[1] = _gyro[2] = 0;
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_spin[0] = _spin[1] = _spin[2] = 0;
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}
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RigidBody::~RigidBody()
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{
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delete[] _masses;
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}
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int RigidBody::addMass(float mass, float* pos)
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{
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// If out of space, reallocate twice as much
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if(_nMasses == _massesAlloced) {
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_massesAlloced *= 2;
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Mass *m2 = new Mass[_massesAlloced];
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2001-12-07 20:00:59 +00:00
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int i;
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for(i=0; i<_nMasses; i++)
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2001-12-01 06:22:24 +00:00
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m2[i] = _masses[i];
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delete[] _masses;
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_masses = m2;
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}
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_masses[_nMasses].m = mass;
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Math::set3(pos, _masses[_nMasses].p);
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return _nMasses++;
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}
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void RigidBody::setMass(int handle, float mass)
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{
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_masses[handle].m = mass;
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}
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void RigidBody::setMass(int handle, float mass, float* pos)
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{
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_masses[handle].m = mass;
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Math::set3(pos, _masses[handle].p);
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}
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int RigidBody::numMasses()
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{
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return _nMasses;
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}
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float RigidBody::getMass(int handle)
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{
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return _masses[handle].m;
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}
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void RigidBody::getMassPosition(int handle, float* out)
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{
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out[0] = _masses[handle].p[0];
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out[1] = _masses[handle].p[1];
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out[2] = _masses[handle].p[2];
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}
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float RigidBody::getTotalMass()
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{
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return _totalMass;
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}
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// Calcualtes the rotational velocity of a particular point. All
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// coordinates are local!
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void RigidBody::pointVelocity(float* pos, float* rot, float* out)
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{
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Math::sub3(pos, _cg, out); // out = pos-cg
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Math::cross3(rot, out, out); // = rot cross (pos-cg)
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}
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void RigidBody::setGyro(float* angularMomentum)
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{
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Math::set3(angularMomentum, _gyro);
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}
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void RigidBody::recalc()
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{
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// Calculate the c.g and total mass:
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_totalMass = 0;
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_cg[0] = _cg[1] = _cg[2] = 0;
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2001-12-07 20:00:59 +00:00
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int i;
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for(i=0; i<_nMasses; i++) {
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2001-12-01 06:22:24 +00:00
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float m = _masses[i].m;
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_totalMass += m;
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_cg[0] += m * _masses[i].p[0];
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_cg[1] += m * _masses[i].p[1];
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_cg[2] += m * _masses[i].p[2];
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}
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Math::mul3(1/_totalMass, _cg, _cg);
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// Now the inertia tensor:
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2001-12-07 20:00:59 +00:00
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for(i=0; i<9; i++)
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_tI[i] = 0;
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2001-12-01 06:22:24 +00:00
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2001-12-07 20:00:59 +00:00
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for(i=0; i<_nMasses; i++) {
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2001-12-01 06:22:24 +00:00
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float m = _masses[i].m;
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float x = _masses[i].p[0] - _cg[0];
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float y = _masses[i].p[1] - _cg[1];
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float z = _masses[i].p[2] - _cg[2];
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float xy = m*x*y; float yz = m*y*z; float zx = m*z*x;
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float x2 = m*x*x; float y2 = m*y*y; float z2 = m*z*z;
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2001-12-07 20:00:59 +00:00
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_tI[0] += y2+z2; _tI[1] -= xy; _tI[2] -= zx;
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_tI[3] -= xy; _tI[4] += x2+z2; _tI[5] -= yz;
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_tI[6] -= zx; _tI[7] -= yz; _tI[8] += x2+y2;
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2001-12-01 06:22:24 +00:00
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}
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// And its inverse
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2001-12-07 20:00:59 +00:00
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Math::invert33(_tI, _invI);
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2001-12-01 06:22:24 +00:00
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}
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void RigidBody::reset()
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{
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_torque[0] = _torque[1] = _torque[2] = 0;
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_force[0] = _force[1] = _force[2] = 0;
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}
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void RigidBody::addForce(float* force)
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{
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Math::add3(_force, force, _force);
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}
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void RigidBody::addTorque(float* torque)
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{
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Math::add3(_torque, torque, _torque);
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}
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void RigidBody::addForce(float* pos, float* force)
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{
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addForce(force);
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// For a force F at position X, the torque about the c.g C is:
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// torque = F cross (C - X)
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float v[3], t[3];
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Math::sub3(_cg, pos, v);
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Math::cross3(force, v, t);
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addTorque(t);
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}
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void RigidBody::setBodySpin(float* rotation)
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{
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Math::set3(rotation, _spin);
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}
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void RigidBody::getCG(float* cgOut)
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{
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Math::set3(_cg, cgOut);
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}
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void RigidBody::getAccel(float* accelOut)
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{
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Math::mul3(1/_totalMass, _force, accelOut);
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}
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void RigidBody::getAccel(float* pos, float* accelOut)
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{
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getAccel(accelOut);
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// Turn the "spin" vector into a normalized spin axis "a" and a
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// radians/sec scalar "rate".
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float a[3];
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float rate = Math::mag3(_spin);
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Math::set3(_spin, a);
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2006-08-14 21:59:44 +00:00
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if (rate !=0 )
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Math::mul3(1/rate, a, a);
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//an else branch is not neccesary. a, which is a=(0,0,0) in the else case, is only used in a dot product
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2001-12-01 06:22:24 +00:00
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float v[3];
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Math::sub3(_cg, pos, v); // v = cg - pos
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Math::mul3(Math::dot3(v, a), a, a); // a = a * (v dot a)
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Math::add3(v, a, v); // v = v + a
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// Now v contains the vector from pos to the rotation axis.
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// Multiply by the square of the rotation rate to get the linear
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// acceleration.
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Math::mul3(rate*rate, v, v);
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Math::add3(v, accelOut, accelOut);
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}
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void RigidBody::getAngularAccel(float* accelOut)
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{
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// Compute "tau" as the externally applied torque, plus the
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// counter-torque due to the internal gyro.
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float tau[3]; // torque
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Math::cross3(_gyro, _spin, tau);
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Math::add3(_torque, tau, tau);
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// Now work the equation of motion. Use "v" as a notational
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// shorthand, as the value isn't an acceleration until the end.
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float *v = accelOut;
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2001-12-07 20:00:59 +00:00
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Math::vmul33(_tI, _spin, v); // v = I*omega
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2001-12-01 06:22:24 +00:00
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Math::cross3(_spin, v, v); // v = omega X I*omega
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Math::add3(tau, v, v); // v = tau + (omega X I*omega)
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Math::vmul33(_invI, v, v); // v = invI*(tau + (omega X I*omega))
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}
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2007-01-10 19:04:59 +00:00
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void RigidBody::getInertiaMatrix(float* inertiaOut)
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{
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// valid only after a call to RigidBody::recalc()
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// See comment at top of RigidBody.hpp on units.
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for(int i=0;i<9;i++)
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{
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inertiaOut[i] = _tI[i];
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}
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}
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2001-12-01 06:22:24 +00:00
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}; // namespace yasim
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