Theorem 9.7.2. There is only one line of curvature that passes through each flat point on a line of flat points, and that line of curvature is orthogonal to the direction of the generator [251].
Proof: By Lemma 9.7.1 the developable surface is
expressed locally as a cubic cylinder at an ordinary inflection line
and more generally in the form of (9.95) at a higher
order contact line. If we rewrite (9.95) in terms of
polar coordinates by substituting
for a fixed radius
we obtain
| (9.97) |
| (9.98) |
If we denote as the angle between the axis and the direction of the nonzero principal curvature in parametric space, can be evaluated as follows. Since the direction of the nonzero principal curvature is orthogonal to the generator (parallel to the local axis), its direction is given by and hence .
We can trace the lines of curvature which pass through the flat points of an inflection line by integrating the initial value problem following the procedure described in Sect. 9.4. The starting points are obtained by slightly shifting outwards in the directions 0 and from the flat points or, equivalently, along the positive and negative local axis.
In generic cases, umbilics are isolated [257]; thus an inflection line, which consists of a line of flat points, is non-generic and therefore unstable. In the following we give a couple of numerical examples that demonstrate the instability of the line of flat points along the inflection line with respect to perturbations.
The example surface is a degree (3-1) integral Bézier patch which is constructed by the method developed in Chalfant [50]. The control points are given by
| = , | = , |
| = , | = , |
| = , | = , |
| = , | = . |
We gradually perturb the control points of the surface and observe the behavior of the lines of curvature which pass through the inflection line as we did in Sect. 9.6. Since the example is a degree (3-1) patch, it has 8 control points. Each control point consists of three Cartesian coordinates , so there are 24 components to be perturbed. We gradually increase the perturbation by increasing in (9.73) from to in steps of .
Figure 9.13 illustrates the behavior of the lines of curvature when the control points are perturbed ( ). We can see from the figure that the entire inflection line, which consists of a line of flat points, disappears. Hence there is no singularity in the net of lines of curvature when a perturbation is induced. The nonzero principal curvatures on both sides of the former inflection line 9.6 meet at right angles near the former inflection line and make a very sharp change in direction (almost a right angle).