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2.4 Frenet-Serret formulae
From (2.20) and (2.44), we found that
(2.53)
(2.54)
From these equations we deduce
(2.55)
In matrix form we can express the differential equations as
(2.56)
Thus,
,
,
are completely determined by the
curvature and torsion of the curve as a function of parameter
.
The equations
,
are called intrinsic equations of the curve. The
formulae (2.56) are known as the Frenet-Serret
formulae and describe the motion of a moving trihedron (
) along the curve.
From these
,
,
the shape of the curve can be determined apart from a translation
and rotation. For arbitrary speed curve the Frenet-Serret formulae are
given by
(2.57)
where
is the parametric speed.
Example 2.4.1
As shown in Example 2.3.1 the intrinsic equations of
circular helix are given by
,
, where
. In this example
we derive the parametric equations of circular helix from these
intrinsic equations. Substituting the intrinsic equations into the
Frenet-Serret equations we obtain
We first differentiate the first equation twice and the second equation once
with respect to
, which yield
where the third equation is used to replace
.
Eliminating
,
,
and recognizing that
, we obtain
the fourth order differential equation
The general solution to this differential equation is given by
where
,
,
and
are the vector
constants determined by the initial conditions.
In this case we assume the following initial conditions
which yield
thus, we have
.
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December 2009