Spiral

In mathematics, a spiral is a curve which emanates from a point, moving further away as it revolves around the point. It is a subtype of whorled patterns, a broad group that also includes concentric objects.
A two-dimensional, or plane, spiral may be easily described using polar coordinates, where the radius r {\displaystyle r} is a monotonic continuous function of angle φ {\displaystyle \varphi } :
The circle would be regarded as a degenerate case (the function not being strictly monotonic, but rather constant).
In x {\displaystyle x} - y {\displaystyle y} -coordinates the curve has the parametric representation:
Some of the most important sorts of two-dimensional spirals include:
An Archimedean spiral is, for example, generated while coiling a carpet.
A hyperbolic spiral appears as image of a helix with a special central projection (see diagram). A hyperbolic spiral is some times called reciproke spiral, because it is the image of an Archimedean spiral with a circle-inversion (see below).
The name logarithmic spiral is due to the equation φ = 1 k ⋅ ln ⁡ r a {\displaystyle \varphi ={\tfrac {1}{k}}\cdot \ln {\tfrac {r}{a}}} . Approximations of this are found in nature.
Spirals which do not fit into this scheme of the first 5 examples:
A Cornu spiral has two asymptotic points. The spiral of Theodorus is a polygon. The Fibonacci Spiral consists of a sequence of circle arcs. The involute of a circle looks like an Archimedean, but is not: see Involute#Examples.
The following considerations are dealing with spirals, which can be described by a polar equation r = r ( φ ) {\displaystyle r=r(\varphi )} , especially for the cases r ( φ ) = a φ n {\displaystyle r(\varphi )=a\varphi ^{n}} (Archimedean, hyperbolic, Fermat's, lituus spirals) and the logarithmic spiral r = a e k φ {\displaystyle r=ae^{k\varphi }} .
The angle α {\displaystyle \alpha } between the spiral tangent and the corresponding polar circle (see diagram) is called angle of the polar slope and tan ⁡ α {\displaystyle \tan \alpha } the polar slope.
From vector calculus in polar coordinates one gets the formula
Hence the slope of the spiral r = a φ n {\displaystyle \;r=a\varphi ^{n}\;} is
In case of an Archimedean spiral ( n = 1 {\displaystyle n=1} ) the polar slope is tan ⁡ α = 1 φ . {\displaystyle \;\tan \alpha ={\tfrac {1}{\varphi }}\ .}
In a logarithmic spiral, tan ⁡ α = k {\displaystyle \ \tan \alpha =k\ } is constant.
The curvature κ {\displaystyle \kappa } of a curve with polar equation r = r ( φ ) {\displaystyle r=r(\varphi )} is
For a spiral with r = a φ n {\displaystyle r=a\varphi ^{n}} one gets
In case of n = 1 {\displaystyle n=1} (Archimedean spiral) κ = φ 2 + 2 a ( φ 2 + 1 ) 3 / 2 {\displaystyle \kappa ={\tfrac {\varphi ^{2}+2}{a(\varphi ^{2}+1)^{3/2}}}} . Only for − 1 < n < 0 {\displaystyle -1<n<0} the spiral has an inflection point.
The curvature of a logarithmic spiral r = a e k φ {\displaystyle \;r=ae^{k\varphi }\;} is κ = 1 r 1 + k 2 . {\displaystyle \;\kappa ={\tfrac {1}{r{\sqrt {1+k^{2}}}}}\;.}
The area of a sector of a curve (see diagram) with polar equation r = r ( φ ) {\displaystyle r=r(\varphi )} is
For a spiral with equation r = a φ n {\displaystyle r=a\varphi ^{n}\;} one gets
The formula for a logarithmic spiral r = a e k φ {\displaystyle \;r=ae^{k\varphi }\;} is A = r ( φ 2 ) 2 − r ( φ 1 ) 2 ) 4 k . {\displaystyle \ A={\tfrac {r(\varphi _{2})^{2}-r(\varphi _{1})^{2})}{4k}}\ .}
The length of an arc of a curve with polar equation r = r ( φ ) {\displaystyle r=r(\varphi )} is
For the spiral r = a φ n {\displaystyle r=a\varphi ^{n}\;} the length is
Not all these integrals can be solved by a suitable table. In case of a Fermat's spiral, the integral can be expressed by elliptic integrals only.
The arc length of a logarithmic spiral r = a e k φ {\displaystyle \;r=ae^{k\varphi }\;} is L = k 2 + 1 k ( r ( φ 2 ) − r ( φ 1 ) ) . {\displaystyle \ L={\tfrac {\sqrt {k^{2}+1}}{k}}{\big (}r(\varphi _{2})-r(\varphi _{1}){\big )}\ .}
The inversion at the unit circle has in polar coordinates the simple description: ( r , φ ) ↦ ( 1 r , φ ) {\displaystyle \ (r,\varphi )\mapsto ({\tfrac {1}{r}},\varphi )\ } .
The function r ( φ ) {\displaystyle r(\varphi )} of a spiral is usually strictly monotonic, continuous and unbounded. For the standard spirals r ( φ ) {\displaystyle r(\varphi )} is either a power function or an exponential function. If one chooses for r ( φ ) {\displaystyle r(\varphi )} a bounded function, the spiral is bounded, too. A suitable bounded function is the arctan function:
Setting r = a arctan ⁡ ( k φ ) {\displaystyle \;r=a\arctan(k\varphi )\;} and the choice k = 0.1 , a = 4 , φ ≥ 0 {\displaystyle \;k=0.1,a=4,\;\varphi \geq 0\;} gives a spiral, that starts at the origin (like an Archimedean spiral) and approaches the circle with radius r = a π / 2 {\displaystyle \;r=a\pi /2\;} (diagram, left).
For r = a ( arctan ⁡ ( k φ ) + π / 2 ) {\displaystyle \;r=a(\arctan(k\varphi )+\pi /2)\;} and k = 0.2 , a = 2 , − ∞ < φ < ∞ {\displaystyle \;k=0.2,a=2,\;-\infty <\varphi <\infty \;} one gets a spiral, that approaches the origin (like a hyperbolic spiral) and approaches the circle with radius r = a π {\displaystyle \;r=a\pi \;} (diagram, right).
Two major definitions of "spiral" in the American Heritage Dictionary are:
The first definition describes a planar curve, that extends in both of the perpendicular directions within its plane; the groove on one side of a gramophone record closely approximates a plane spiral (and it is by the finite width and depth of the groove, but not by the wider spacing between than within tracks, that it falls short of being a perfect example); note that successive loops differ in diameter. In another example, the "center lines" of the arms of a spiral galaxy trace logarithmic spirals.
The second definition includes two kinds of 3-dimensional relatives of spirals:
In the side picture, the black curve at the bottom is an Archimedean spiral, while the green curve is a helix. The curve shown in red is a conical spiral.
Two well-known spiral space curves are conical spirals and spherical spirals, defined below. Another instance of space spirals is the toroidal spiral. A spiral wound around a helix, also known as double-twisted helix, represents objects such as coiled coil filaments.
If in the x {\displaystyle x} - y {\displaystyle y} -plane a spiral with parametric representation
is given, then there can be added a third coordinate z ( φ ) {\displaystyle z(\varphi )} , such that the now space curve lies on the cone with equation m ( x 2 + y 2 ) = ( z − z 0 ) 2 , m > 0 {\displaystyle \;m(x^{2}+y^{2})=(z-z_{0})^{2}\ ,\ m>0\;} :
Spirals based on this procedure are called conical spirals.
Starting with an archimedean spiral r ( φ ) = a φ {\displaystyle \;r(\varphi )=a\varphi \;} one gets the conical spiral (see diagram)
Any cylindrical map projection can be used as the basis for a spherical spiral: draw a straight line on the map and find its inverse projection on the sphere, a kind of spherical curve.
One of the most basic families of spherical spirals is the Clelia curves, which project to straight lines on an equirectangular projection. These are curves for which longitude and colatitude are in a linear relationship, analogous to Archimedean spirals in the plane; under the azimuthal equidistant projection a Clelia curve projects to a planar Archimedean spiral.
If one represents a unit sphere by spherical coordinates
then setting the linear dependency φ = c θ {\displaystyle \varphi =c\theta } for the angle coordinates gives a parametric curve in terms of parameter ⁠ θ {\displaystyle \theta } ⁠,
Another family of spherical spirals is the rhumb lines or loxodromes, that project to straight lines on the Mercator projection. These are the trajectories traced by a ship traveling with constant bearing. Any loxodrome (except for the meridians and parallels) spirals infinitely around either pole, closer and closer each time, unlike a Clelia curve which maintains uniform spacing in colatitude. Under stereographic projection, a loxodrome projects to a logarithmic spiral in the plane.
The study of spirals in nature has a long history. Christopher Wren observed that many shells form a logarithmic spiral; Jan Swammerdam observed the common mathematical characteristics of a wide range of shells from Helix to Spirula; and Henry Nottidge Moseley described the mathematics of univalve shells. D’Arcy Wentworth Thompson's On Growth and Form gives extensive treatment to these spirals. He describes how shells are formed by rotating a closed curve around a fixed axis: the shape of the curve remains fixed, but its size grows in a geometric progression. In some shells, such as Nautilus and ammonites, the generating curve revolves in a plane perpendicular to the axis and the shell will form a planar discoid shape. In others it follows a skew path forming a helico-spiral pattern. Thompson also studied spirals occurring in horns, teeth, claws and plants.
A model for the pattern of florets in the head of a sunflower was proposed by H. Vogel. This has the form
where n is the index number of the floret and c is a constant scaling factor, and is a form of Fermat's spiral. The angle 137.5° is the golden angle which is related to the golden ratio and gives a close packing of florets.
Spirals in plants and animals are frequently described as whorls. This is also the name given to spiral shaped fingerprints.
The Celtic triple-spiral is in fact a pre-Celtic symbol. It is carved into the rock of a stone lozenge near the main entrance of the prehistoric Newgrange monument in County Meath, Ireland. Newgrange was built around 3200 BCE, predating the Celts; triple spirals were carved at least 2,500 years before the Celts reached Ireland, but have long since become part of Celtic culture. The triskelion symbol, consisting of three interlocked spirals or three bent human legs, appears in many early cultures: examples include Mycenaean vessels, coinage from Lycia, staters of Pamphylia (at Aspendos, 370–333 BC) and Pisidia, as well as the heraldic emblem on warriors' shields depicted on Greek pottery.
Spirals occur commonly in pre-Columbian art in Latin and Central America. The more than 1,400 petroglyphs (rock engravings) in Las Plazuelas, Guanajuato Mexico, dating 750-1200 AD, predominantly depict spirals, dot figures and scale models. In Colombia, monkeys, frog and lizard-like figures depicted in petroglyphs or as gold offering-figures frequently include spirals, for example on the palms of hands. In Lower Central America, spirals along with circles, wavy lines, crosses and points are universal petroglyph characters. Spirals also appear among the Nazca Lines in the coastal desert of Peru, dating from 200 BC to 500 AD. The geoglyphs number in the thousands and depict animals, plants and geometric motifs, including spirals.
Spirals are also a symbol of hypnosis, stemming from the cliché of people and cartoon characters being hypnotized by staring into a spinning spiral (one example being Kaa in Disney's The Jungle Book). They are also used as a symbol of dizziness, where the eyes of a cartoon character, especially in anime and manga, will turn into spirals to suggest that they are dizzy or dazed. The spiral is also found in structures as small as the double helix of DNA and as large as a galaxy. Due to this frequent natural occurrence, the spiral is the official symbol of the World Pantheist Movement. The spiral is also a symbol of the dialectic process and of Dialectical monism.
The spiral has inspired artists throughout the ages. Among the most famous of spiral-inspired art is Robert Smithson's earthwork, "Spiral Jetty", at the Great Salt Lake in Utah. The spiral theme is also present in David Wood's Spiral Resonance Field at the Balloon Museum in Albuquerque, as well as in the critically acclaimed Nine Inch Nails 1994 concept album The Downward Spiral. The Spiral is also a prominent theme in the anime Gurren Lagann, where it represents a philosophy and way of life. It also central in Mario Merz and Andy Goldsworthy's work. The spiral is the central theme of the horror manga Uzumaki by Junji Ito, where a small coastal town is afflicted by a curse involving spirals.