Given a curve
parameterized by arc length, we want to describe the
bending and twisting of the curve at a point. Starting with the unit tangent
vector
, we can examine the vector
. This is a vector which we break into two parts: a scalar
curvature
and a vector normal. Hence the curvature is
defined as
and the normal is uniquely defined if
. The curvature describes how the curve pulls away from the tangent.
The inverse of the curvature
is called the radius of
curvature and describes the size of a circle with the same curvature.
The plane that contains
and
is called the
osculating plane. If a curve is completely contained in a plane, then
the osculating plane at every point coincides with the containing plane. For
this section, we will assume that
so that the normal is defined
everywhere.
The unit binormal vector
is the second
direction in which the curve can bend and is perpendicular to the osculating
plane by definition2.1. The rate of change of
describes how the osculating planes of neighbouring points differ, or put
another way, how the curve pulls out of the osculating plane.
It is useful to know how the three vectors change with changes of parameter.
By definition, we have
. For the binormal, we have
| (2.5) | ||
| (2.6) | ||
| (2.7) |
| (2.8) | ||
| (2.9) | ||
| (2.10) |
To summarize, the behaviour of a arc length parameterized curve can be
characterized by three orthonormal vectors, namely the tangent
, the
normal
and the binormal
, and two scalars, namely the curvature
and the torsion
. The frame defined by the three vectors and
the point
is called the Frenet frame.
The fundamental theorem of the local theory of curves says that all
curves with identical
and
are identical up to rigid
transformations. That is, the curvature and torsion uniquely characterize the
local behaviour of a curve.