本文整理汇总了C++中math::Vector::nrm方法的典型用法代码示例。如果您正苦于以下问题：C++ Vector::nrm方法的具体用法？C++ Vector::nrm怎么用？C++ Vector::nrm使用的例子？那么, 这里精选的方法代码示例或许可以为您提供帮助。您也可以进一步了解该方法所在类math::Vector的用法示例。
在下文中一共展示了Vector::nrm方法的3个代码示例，这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞，您的评价将有助于系统推荐出更棒的C++代码示例。
示例1: ray_rod
/*! \brief A ray-rod intersection test.
A rod is a cylinder which is not infinite, but of limited
length. The cylinder is defined using a single base vertex at
the center of the bottom circular face and an axial vector
pointing from the base vertex to the top vertex. This test
ignores the back face of the rod. It is used to detect when a
ray will enter a rod.
\param T The origin of the ray relative to the base vertex.
\param D The direction/velocity of the ray.
\param A The axial vector of the rod.
\param r Radius of the rod.
\return The time until the intersection, or HUGE_VAL if no intersection.
*/
inline double ray_rod(math::Vector T, math::Vector D, const math::Vector& A, const double r)
{
double t = ray_cylinder(T, D, A / A.nrm(), r);
double Tproj = ((T + t * D) | A);
if ((Tproj < 0) || (Tproj > A.nrm2())) return HUGE_VAL;
return t;
}示例2: ray_inv_rod
/*! \brief A ray-inverse_rod intersection test.
A rod is a cylinder which is not infinite, but of limited
length. An inverse rod is used to test when a ray will exit a
rod. The cylinder is defined using a single base vertex at the
center of the bottom circular face and an axial vector
pointing from the base vertex to the top vertex. This test
ignores the back face of the rod.
\param T The origin of the ray relative to the base vertex.
\param D The direction/velocity of the ray.
\param A The axial vector of the inverse rod.
\param r Radius of the inverse rod.
\tparam always_intersect If true, this will ensure that glancing
ray's never escape the enclosing sphere by returning the time
when the ray is nearest the sphere if the ray does not intersect
the sphere.
\return The time until the intersection, or HUGE_VAL if no intersection.
*/
inline double ray_inv_rod(math::Vector T, math::Vector D, const math::Vector& A, const double r)
{
double t = ray_inv_cylinder(T, D, A / A.nrm(), r);
M_throw() << "Confirm that this function is correct";
double Tproj = ((T + t * D) | A);
if ((Tproj < 0) || (Tproj > A.nrm2())) return HUGE_VAL;
return t;
}示例3:
OffcentreSpheresOverlapFunction(const math::Vector& rij, const math::Vector& vij, const math::Vector& omegai, const math::Vector& omegaj,
const math::Vector& nu1, const math::Vector& nu2, const double diameter1, const double diameter2,
const double maxdist, const double t, const double invgamma, const double t_min, const double t_max):
w1(omegai), w2(omegaj), u1(nu1), u2(nu2), r12(rij), v12(vij), _diameter1(diameter1), _diameter2(diameter2), _invgamma(invgamma), _t(t), _t_min(t_min), _t_max(t_max)
{
double Gmax = std::max(1 + t * invgamma, 1 + (t + t_max) * invgamma);
const double sigmaij = 0.5 * (_diameter1 + _diameter2);
const double sigmaij2 = sigmaij * sigmaij;
double magw1 = w1.nrm(), magw2 = w2.nrm();
double rijmax = Gmax * std::max(maxdist, rij.nrm());
#ifdef MAGNET_DEBUG
if (rij.nrm() > 1.0001 * maxdist)
std::cout << "WARNING!: Particle separation is larger than the maximum specified. " <<rij.nrm() << ">" << maxdist << "\n";
#endif
double magu1 = u1.nrm(), magu2 = u2.nrm();
double vijmax = v12.nrm() + Gmax * (magu1 * magw1 + magu2 * magw2) + std::abs(invgamma) * (magu1 + magu2);
double aijmax = Gmax * (magu1 * magw1 * magw1 + magu2 * magw2 * magw2) + 2 * std::abs(invgamma) * (magu1 * magw1 + magu2 * magw2);
double dotaijmax = Gmax * (magu1 * magw1 * magw1 * magw1 + magu2 * magw2 * magw2 * magw2) + 3 * std::abs(invgamma) * (magu1 * magw1 * magw1 + magu2 * magw2 * magw2);
_f1max = 2 * rijmax * vijmax + 2 * Gmax * std::abs(invgamma) * sigmaij2;
_f2max = 2 * vijmax * vijmax + 2 * rijmax * aijmax + 2 * invgamma * invgamma * sigmaij2;
_f3max = 6 * vijmax * aijmax + 2 * rijmax * dotaijmax;
}