The second fundamental form is similar to the first fundamental form
(sec:FirstFundamentalForm), except that it relates a vector
in
the tangent plane to the change in normal in the direction of
.
Specifically, the second fundamental form or shape operator
at a point
is defined as
| (2.30) |
To see how this might be true, consider a regular arc length-parameterized
curve
on the surface. The field of normals restricted to the
curve is also a function of
:
. Since the normal
is always perpendicular to the tangent plane, we have
, which we can differentiate to obtain
. Therefore
| (2.31) | ||
| (2.32) | ||
| (2.33) | ||
| (2.34) | ||
| (2.35) |
Copyright © 2005 Adrian Secord. All rights reserved.