A **hyperbolic spiral** is a plane curve, which can be described in polar coordinates by the equation

of a hyperbola. Because it can be generated by a circle inversion of an Archimedean spiral, it is called **Reciprocal spiral**, too.^{[1]}^{[2]}

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 a pitch angle that increases with distance from its center, unlike the logarithmic spiral (in which the angle is constant) or Archimedean spiral (in which it decreases with distance). For this reason, it has been used to model the shapes of spiral galaxies, which in some cases similarly have a similarly increasing pitch angle. However, this model does not provide a good fit to the shapes of all spiral galaxies.^{[3]}^{[4]}

the hyperbolic spiral with the polar equation

can be represented in Cartesian coordinates (*x* = *r* cos *φ*, *y* = *r* sin *φ*) by

The hyperbola has in the rφ-plane the coordinate axes as asymptotes. The hyperbolic spiral (in the xy-plane) approaches for *φ* → ±∞ the origin as asymptotic point. For *φ* → ±0 the curve has an asymptotic line (see next section).

From the polar equation and *φ* = *a*/*r*, *r* = √*x*^{2} + *y*^{2} one gets a representation by an *equation*:

Because

the curve has an *asymptote* with equation *y* = *a*.

From vector calculus in polar coordinates one gets the formula tan *α* = *r*′/*r* for the *polar slope* and its angle α between the tangent of a curve and the tangent of the corresponding polar circle.

For the hyperbolic spiral *r* = *a*/*φ* the *polar slope* is

The curvature of a curve with polar equation *r* = *r*(*φ*) is

From the equation *r* = *a*/*φ* and the derivatives *r*′ = −*a*/*φ*^{2} and *r*″ = 2*a*/*φ*^{3} one gets the *curvature* of a hyperbolic spiral:

The length of the arc of a hyperbolic spiral between (*r*(*φ*_{1}), *φ*_{1}) and (*r*(*φ*_{2}), *φ*_{2}) can be calculated by the integral:

The area of a sector (see diagram above) of a hyperbolic spiral with equation *r* = *a*/*φ* is:

The inversion at the unit circle has in polar coordinates the simple description: (*r*, *φ*) ↦ (1/*r*, *φ*).

The image of an Archimedean spiral *r* = *φ*/*a* with a circle inversion is the hyperbolic spiral with equation *r* = *a*/*φ*. At *φ* = *a* the two curves intersect at a fixed point on the unit circle.

The osculating circle of the Archimedean spiral *r* = *φ*/*a* at the origin has radius *ρ*_{0} = 1/2*a* (see Archimedean spiral) and center (*0*, *ρ*_{0}). The image of this circle is the line *y* = *a* (see circle inversion). Hence the preimage of the asymptote of the hyperbolic spiral with the inversion of the Archimedean spiral is the osculating circle of the Archimedean spiral at the origin.

*Example:*The diagram shows an example with*a*=*π*.

Consider the central projection from point *C*_{0} = (0, 0, *d*) onto the image plane *z* = 0. This will map a point (*x*, *y*, *z*) to the point *d*/*d* − *z*(*x*, *y*).

The image under this projection of the helix with parametric representation

is the curve

with the polar equation

which describes a hyperbolic spiral.

For parameter *t*_{0} = *d*/*c* the hyperbolic spiral has a pole and the helix intersects the plane *z* = *d* at a point *V*_{0}. One can check by calculation that the image of the helix as it approaches *V*_{0} is the asymptote of the hyperbolic spiral.