A **spiral** is a curve which turns around some central point or axis, getting progressively closer to or farther from it, depending on which way you follow the curve.

Table of contents |

2 Three-dimensional spirals |

A two-dimensional spiral may be described using
polar coordinates by saying that *r* is a continuous monotonic function of θ. The circle would be regarded as a degenerate case (the function not being strictly monotonic, but rather constant).

Some of the more important sorts of two-dimensional spirals include:

- The Archimedean spiral —
*r*=*a*+*b*θ - The hyperbolic spiral —
*r*=*a*/θ - The logarithmic spiral —
*r*=*ab*^{θ}; approximations of this are found in nature - Fermat's spiral —
*r*= θ^{1/2} - The lituus —
*r*= 1/θ^{1/2}

As in the two-dimensional case, *r* is a continuous monotonic function of θ.

For simple 3-d spirals, the third variable, *h* (height), is also a continuous, monotonic function of θ.

For compound 3-d spirals, such as the *spherical spiral* described below,
*h* increases with θ on one side of a point, and decreases with θ on the other side.

The helix can be viewed as a kind of three-dimensional spiral.

A *spherical spiral* is the curve on a sphere traced by a ship traveling from one pole to the other while keeping a fixed angle (but not a right angle) with respect to the meridians of longitude (cf. rhumb line). The curve has an infinite number of revolutions, with the distance between them decreasing as the curve approaches either of the poles.