Hyperbolic spiral

From Wikipedia, the free encyclopedia
Jump to navigation Jump to search
Hyperbolic spiral for a = 2

A hyperbolic spiral is a transcendental plane curve also known as a reciprocal spiral.[1] A hyperbolic spiral is the inverse of an Archimedean spiral[2] and is a type of Cotes' spiral.

Pierre Varignon first studied the curve in 1704.[2] Later Johann Bernoulli and Roger Cotes worked on the curve as well.


The hyperbolic spiral has the polar equation:

It begins at an infinite distance from the pole in the center (for θ starting from zero r = a/θ starts from infinity), and it winds faster and faster around as it approaches the pole; the distance from any point to the pole, following the curve, is infinite. Applying the transformation from the polar coordinate system:

leads to the following parametric representation in Cartesian coordinates:

where the parameter t is an equivalent of the polar coordinate θ.



The spiral has an asymptote at y = a: for t approaching zero the ordinate approaches a, while the abscissa grows to infinity:


Using the representation of the hyperbolic spiral in polar coordinates, the curvature can be found by



Then the curvature at reduces to

The curvature tends to infinity as tends to infinity. For values of between 0 and 1, the curvature increases exponentially, and for values greater than 1, the curvature increases at an approximately linear rate with respect to the angle.


The polar tangential angle of the hyperbolic spiral is


  1. ^ Bowser, Edward Albert (1880), An Elementary Treatise on Analytic Geometry: Embracing Plane Geometry and an Introduction to Geometry of Three Dimensions (4th ed.), D. Van Nostrand, p. 232.
  2. ^ a b Lawrence, J. Dennis (2013), A Catalog of Special Plane Curves, Dover Books on Mathematics, Courier Dover Publications, p. 186, ISBN 9780486167664.

External links[edit]