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Sinusoidal spiral : ウィキペディア英語版
Sinusoidal spiral

In geometry, the sinusoidal spirals are a family of curves defined by the equation in polar coordinates
:r^n = a^n \cos(n \theta)\,
where ''a'' is a nonzero constant and ''n'' is a rational number other than 0. With a rotation about the origin, this can also be written
:r^n = a^n \sin(n \theta).\,
The term "spiral" is a misnomer, because they are not actually spirals, and often have a flower-like shape. Many well known curves are sinusoidal spirals including:
* Equilateral hyperbola (''n'' = −2)
* Line (''n'' = −1)
* Parabola (''n'' = −1/2)
* Tschirnhausen cubic (''n'' = −1/3)
* Cayley's sextet (''n'' = 1/3)
* Cardioid (''n'' = 1/2)
* Circle (''n'' = 1)
* Lemniscate of Bernoulli (''n'' = 2)
The curves were first studied by Colin Maclaurin.
==Equations==
Differentiating
:r^n = a^n \cos(n \theta)\,
and eliminating ''a'' produces a differential equation for ''r'' and θ:
:\frac\cos n\theta + r\sin n\theta =0.
Then
:\left(\frac,\ r\frac\right)\cos n\theta \frac
= \left(-r\sin n\theta ,\ r \cos n\theta \right)
= r\left(-\sin n\theta ,\ \cos n\theta \right)
which implies that the polar tangential angle is
:\psi = n\theta \pm \pi/2
and so the tangential angle is
:\varphi = (n+1)\theta \pm \pi/2.
(The sign here is positive if ''r'' and cos ''n''θ have the same sign and negative otherwise.)
The unit tangent vector,
:\left(\frac,\ r\frac\right),
has length one, so comparing the magnitude of the vectors on each side of the above equation gives
:\frac = r \cos^ n\theta = a \cos^} n\theta.
In particular, the length of a single loop when n>0 is:
:a\int_}^} \cos^} n\theta\ d\theta
The curvature is given by
:\frac = (n+1)\frac = \frac \cos^} n\theta.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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