7.3 Center and radius of curvature 437
where n is the unit normal obtained by rotating t clockwise through the angle
a/2, ds/dt is the speed of the particle, and K is the curvature dO/ds of C. Show
that writing the formula v = IvIt in the form
(3)
and differentiating give
V_ds
Wt t
2
(4) a = at =ate t + as at
and that use of (2) then gives
(5) a - atit+(dt)2Kn.
Remark: This elegant formula gives the normal (or transverse) and tangential
scalar components of the acceleration in terms of the speed and rate of change of
the speed of the particle. The simplest applications involve the case in which the
particle moves along the curve with constant speed v so that ds/dt = a. and
d2s/dt2 = 0 at each time. In this case, (5) reduces to the simple but important
formula
(6) a = v2Kn.
If K = 0, then a = 0. If K 0 0, then a has magnitude a21 K1 or a2/p (where p
is the radius of curvature) and is directed toward the center of curvature. Use of
(6) and the formula F = ma gives the force required to propel a particle of mass m
along a curve C with constant speed v.
18 Let C be a simple closed convex curve which could, for example, be a
famous "triangular roller" composed of the three vertices of an equilateral tri-
angle together with three circular arcs of which each has its center at one vertex
and contains the other two vertices. Let R be a rod (or line segment) whose
length L is small enough to permit the rod to be "slid around" C in such a way
that its two ends both remain on C. It is easy to presume, as has sometimes
been done in "proofs" of the "Holditch theorem," that each point P on R must
traverse a simple closed convex curve Cr as R slides around C. Persons having
a compass, a straightedge like the edge of a sheet of paper upon which marks
can be placed, and some spare time at their disposal can sketch interesting
figures. Surprises await those who let C be a triangular roller, let the length L
of the rod R be equal to or only a bit less than the distance between two vertices
of the equilateral triangle, and let P be the mid-point of L.