Fermat's spiral

Fermat's spiral
A Fermat's spiral or parabolic spiral is a plane curve with the property that the area between any two consecutive full turns around the spiral is invariant. As a result, the distance between turns grows in inverse proportion to their distance from the spiral center, contrasting with the Archimedean spiral (for which this distance is invariant) and the logarithmic spiral (for which the distance between turns is proportional to the distance from the center). Fermat spirals are named after Pierre de Fermat.
Their applications include curvature continuous blending of curves, modeling plant growth and the shapes of certain spiral galaxies, and the design of variable capacitors, solar power reflector arrays, and cyclotrons.
Coordinate representation
Polar
The representation of the Fermat spiral in polar coordinates is given by the equation
for .
The two choices of sign give the two branches of the spiral, which meet smoothly at the origin. If the same variables were reinterpreted as Cartesian coordinates, this would be the equation of a parabola with horizontal axis, which again has two branches above and below the axis, meeting at the origin.
Cartesian
The Fermat spiral with polar equation
can be converted to the Cartesian coordinates by using the standard conversion formulas and . Using the polar equation for the spiral to eliminate from these conversions produces parametric equations for one branch of the curve:
and the second one
They generate the points of branches of the curve as the parameter ranges over the positive real numbers.
For any generated in this way, dividing by cancels the parts of the parametric equations, leaving the simpler equation . From this equation, substituting by (a rearranged form of the polar equation for the spiral) and then substituting by (the conversion from Cartesian to polar) leaves an equation for the Fermat spiral in terms of only and :
Because the sign of is lost when it is squared, this equation covers both branches of the curve.
Geometric properties
Division of the plane
A complete Fermat's spiral (both branches) is a smooth double point free curve, in contrast with the Archimedean and hyperbolic spiral. Like a line or circle or parabola, it divides the plane into two connected regions.
Polar slope
From vector calculus in polar coordinates one gets the formula
for the polar slope and its angle between the tangent of a curve and the corresponding polar circle (see diagram).
For Fermat's spiral one gets
Hence the slope angle is monotonely decreasing.
Curvature
From the formula
for the curvature of a curve with polar equation and its derivatives
one gets the curvature of a Fermat's spiral:
At the origin the curvature is 0. Hence the complete curve has at the origin an inflection point and the -axis is its tangent there.
Area between arcs
The area of a sector of Fermat's spiral between two points and is
After raising both angles by one gets
Hence the area of the region between two neighboring arcs is
only depends on the difference of the two angles, not on the angles themselves.
For the example shown in the diagram, all neighboring stripes have the same area: .
This property is used in electrical engineering for the construction of variable capacitors.
Special case due to Fermat
In 1636, Fermat wrote a letter to Marin Mersenne which contains the following special case:
Let ; then the area of the black region (see diagram) is , which is half of the area of the circle with radius . The regions between neighboring curves (white, blue, yellow) have the same area . Hence:
The area between two arcs of the spiral after a full turn equals the area of the circle .
Arc length
The length of the arc of Fermat's spiral between two points can be calculated by the integral:
This integral leads to an elliptical integral, which can be solved numerically.
The arc length of the positive branch of the Fermat's spiral from the origin can also be defined by hypergeometric functions and the incomplete beta function :
Circle inversion
The inversion at the unit circle has in polar coordinates the simple description .
The image of Fermat's spiral under the inversion at the unit circle is a lituus spiral with polar equation When , both curves intersect at a fixed point on the unit circle.
The tangent (-axis) at the inflection point (origin) of Fermat's spiral is mapped onto itself and is the asymptotic line of the lituus spiral.
The golden ratio and the golden angle
In disc phyllotaxis, as in the sunflower and daisy, the mesh of spirals occurs in Fibonacci numbers because divergence (angle of succession in a single spiral arrangement) approaches the golden ratio. The shape of the spirals depends on the growth of the elements generated sequentially. In mature-disc phyllotaxis, when all the elements are the same size, the shape of the spirals is that of Fermat spirals—ideally. That is because Fermat's spiral traverses equal annuli in equal turns. The full model proposed by H. Vogel in 1979 is
where is the angle, is the radius or distance from the center, and is the index number of the floret and is a constant scaling factor. The angle 137.508° is the golden angle which is approximated by ratios of Fibonacci numbers.
The resulting spiral pattern of unit disks should be distinguished from the Doyle spirals, patterns formed by tangent disks of geometrically increasing radii placed on logarithmic spirals.
Solar plants
Fermat's spiral has also been found to be an efficient layout for the mirrors of concentrated solar power plants.
See also
List of spirals
Patterns in nature
Spiral of Theodorus
References
Further reading
External links
Online exploration using JSXGraph (JavaScript)
Fermat's Natural Spirals, in sciencenews.org
Spirals