Hyperbolic Spiral
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A hyperbolic spiral is a
plane curve In mathematics, a plane curve is a curve in a plane that may be either a Euclidean plane, an affine plane or a projective plane. The most frequently studied cases are smooth plane curves (including piecewise smooth plane curves), and algebraic ...
, which can be described in polar coordinates by the equation :r=\frac of a hyperbola. Because it can be generated by a circle inversion of an Archimedean spiral, it is called Reciprocal spiral, too.. Pierre Varignon first studied the curve in 1704. Later
Johann Bernoulli Johann Bernoulli (also known as Jean or John; – 1 January 1748) was a Swiss mathematician and was one of the many prominent mathematicians in the Bernoulli family. He is known for his contributions to infinitesimal calculus and educating Le ...
and
Roger Cotes Roger Cotes (10 July 1682 – 5 June 1716) was an English mathematician, known for working closely with Isaac Newton by proofreading the second edition of his famous book, the '' Principia'', before publication. He also invented the quadratur ...
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 an increasing pitch angle. However, this model does not provide a good fit to the shapes of all spiral galaxies.


In cartesian coordinates

the hyperbolic spiral with the polar equation :r=\frac a \varphi ,\quad \varphi \ne 0 can be represented in Cartesian coordinates by :x = a \frac \varphi, \qquad y = a \frac \varphi ,\quad \varphi \ne 0. The hyperbola has in the -plane the coordinate axes as asymptotes. The hyperbolic spiral (in the -plane) approaches for the origin as asymptotic point. For the curve has an asymptotic line (see next section). From the polar equation and one gets a representation by an ''equation'': : \frac=\tan\left(\frac\right) .


Geometric properties


Asymptote

Because :\lim_x = a\lim_ \frac \varphi =\infty,\qquad \lim_y = a\lim_ \frac \varphi = a the curve has an ''asymptote'' with equation .


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 tangent of the corresponding polar circle. For the hyperbolic spiral the ''polar slope'' is : \tan\alpha=-\frac.


Curvature

The curvature of a curve with polar equation is :\kappa = \frac . From the equation and the derivatives and one gets the ''curvature'' of a hyperbolic spiral: : \kappa(\varphi) = \frac.


Arc length

The length of the arc of a hyperbolic spiral between and can be calculated by the integral: :\begin L&=\int_^\sqrt\,d\varphi=\cdots \\ &=a \int_^\frac\,d\varphi \\ &= a\left \frac+\ln\left(\varphi+\sqrt\right)\right^ . \end


Sector area

The area of a sector (see diagram above) of a hyperbolic spiral with equation is: :\begin A&=\frac12\int_^ r(\varphi)^2\, d\varphi\\ &=\frac12\int_^\frac\, d\varphi\\ &= \frac\left(\frac-\frac\right)\\ &=\frac\bigl(r(\varphi_1)-r(\varphi_2)\bigr) . \end


Inversion

The inversion at the unit circle has in polar coordinates the simple description: . The image of an Archimedean spiral with a circle inversion is the hyperbolic spiral with equation . At the two curves intersect at a fixed point on the unit circle. The
osculating circle In differential geometry of curves, the osculating circle of a sufficiently smooth plane curve at a given point ''p'' on the curve has been traditionally defined as the circle passing through ''p'' and a pair of additional points on the curve i ...
of the Archimedean spiral at the origin has radius (see Archimedean spiral) and center . The image of this circle is the line (see
circle inversion A circle is a shape consisting of all points in a plane that are at a given distance from a given point, the centre. Equivalently, it is the curve traced out by a point that moves in a plane so that its distance from a given point is const ...
). 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 .


Central projection of a helix

Consider the central projection from point onto the image plane . This will map a point to the point . The image under this projection of the helix with parametric representation :(r\cos t, r\sin t, ct),\quad c\neq 0, is the curve :\frac(\cos t,\sin t) with the polar equation :\rho=\frac, which describes a hyperbolic spiral. For parameter the hyperbolic spiral has a pole and the helix intersects the plane at a point . One can check by calculation that the image of the helix as it approaches is the asymptote of the hyperbolic spiral.


References

* Hans-Jochen Bartsch, Michael Sachs: ''Taschenbuch mathematischer Formeln für Ingenieure und Naturwissenschaftler'', Carl Hanser Verlag, 2018, , 9783446457072, S. 410. * Kinko Tsuji, Stefan C. Müller: ''Spirals and Vortices: In Culture, Nature, and Science'', Springer, 2019, , 9783030057985, S. 96. * Pierre Varignon
''Nouvelle formation de Spirales – exemple II'', Mémoires de l’Académie des sciences de l’Institut de France, 1704, pp. 94–103.
*
Friedrich Grelle Friedrich may refer to: Names *Friedrich (surname), people with the surname ''Friedrich'' *Friedrich (given name), people with the given name ''Friedrich'' Other *Friedrich (board game), a board game about Frederick the Great and the Seven Years' ...
: ''Analytische Geometrie der Ebene'', Verlag F. Brecke, 186
hyperbolische Spirale
S. 215. * Jakob Philipp Kulik: ''Lehrbuch der höhern Analysis, Band 2'', In Commiss. bei Kronberger u. Rziwnatz, 1844
Spirallinien
S. 222.


External links

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{{Spirals Spirals pt:Espiral logarítmica