The curvature
of Euler´s spiral is linearly related to its arc length ^{1)}.
When the path of the curve is followed with an uniform velocity, the speed of
rotation is linear (in time). That's why the curve with the reverse relation is
called the anticlothoid. Most authors present the
curve´s formula in a parametric form:
The formulas under the integral can also be written as the Bessel
functions J_{1/2} (for y) and J_{1/2} (for x).
The spiral, the x and y component
are both a Fresnel integral of a square root.
It was the famous Leonhard Euler who investigated the curve as first (in 1744).
Other names for the spiral are clothoid
and spiral of Cornu or Cornu spiral.
It was the French physicist Marie Alfred Cornu (18411902)
who used the spiral to describe diffraction from the edge of a halfplane.
In the early days of railways it was perfectly adequate to form the railways
with series of straight lines and flat circular curves. When speeds increased
the need developed for a more gradual increase in radius of curvature R
concomitant with an elevation of the outer rail, so that the transition to the
circular curve became smooth.
The clothoid makes a perfect transition spiral.
as its curvature increases linearly with the distance along the spiral.
A first order approximation of this spiral is the cubic spiral.
For the same reason the spiral is used in ship design, specifying the curvature distribution of an
arc of a plane curve while drawing a ship.
To limit the g forces in a looping in a roller coaster, often a clothoid curve is used instead of a circular curve.
This has been patented by Edwin Prescott, in 1901.
Read an interesting mathematical discussion on roller coaster loop shapes.
A generalization of the cuerve can be made to curves where the curvature is a polynomial in s:
the polynomial spiral.
notes ^{1)} dφ/ds = 2a^{2}s leads to φ(s) = (as)^{2}, so that
dx/ds = cos(as)^{2} and dy/ds = sin(as)^{2} which leads to the given integrals.
