“…To deal with this problem, we equivalently reformulate w 2 as an appropriate eigenvector of M. This eigenvector does not vanish along the vortex core line, but since eigenvectors have no orientation, an orientation-free integration of f is necessary here as well. 4 . To get the starting points for the first case, we search for the intersections of the PV lines with the boundary of D: for the boundary face x = x min , we search for all points (y, z) with s(x min , y, z) = (0, 0, 0) T .…”