Conical coordinates

Coordinate surfaces of the conical coordinates. The constants b and c were chosen as 1 and 2, respectively. The red sphere represents r = 2, the blue elliptic cone aligned with the vertical z-axis represents μ=cosh(1) and the yellow elliptic cone aligned with the (green) x-axis corresponds to ν2 = 2/3. The three surfaces intersect at the point P (shown as a black sphere) with Cartesian coordinates roughly (1.26, -0.78, 1.34). The elliptic cones intersect the sphere in taco-shaped curves.

Conical coordinates are a three-dimensional orthogonal coordinate system consisting of concentric spheres (described by their radius r) and by two families of perpendicular cones, aligned along the z- and x-axes, respectively.

Basic definitions

The conical coordinates (r, \mu, \nu) are defined by


x = \frac{r\mu\nu}{bc}

y = \frac{r}{b} \sqrt{\frac{\left( \mu^{2} - b^{2} \right) \left( \nu^{2} - b^{2} \right)}{\left( b^{2} - c^{2} \right)} }

z = \frac{r}{c} \sqrt{\frac{\left( \mu^{2} - c^{2} \right) \left( \nu^{2} - c^{2} \right)}{\left( c^{2} - b^{2} \right)} }

with the following limitations on the coordinates


\nu^{2} < c^{2} < \mu^{2} < b^{2}.

Surfaces of constant r are spheres of that radius centered on the origin


x^{2} + y^{2} + z^{2} = r^{2},

whereas surfaces of constant \mu and \nu are mutually perpendicular cones


\frac{x^{2}}{\mu^{2}} + \frac{y^{2}}{\mu^{2} + b^{2}} + \frac{z^{2}}{\mu^{2} - c^{2}} = 0

and


\frac{x^{2}}{\nu^{2}} + \frac{y^{2}}{\nu^{2} - b^{2}} + \frac{z^{2}}{\nu^{2} + c^{2}} = 0.

In this coordinate system, both Laplace's equation and the Helmholtz equation are separable.

Scale factors

The scale factor for the radius r is one (hr = 1), as in spherical coordinates. The scale factors for the two conical coordinates are


h_{\mu} = r \sqrt{\frac{\mu^{2} - \nu^{2}}{\left( b^{2} - \mu^{2} \right) \left( \mu^{2} - c^{2} \right)}}

and


h_{\nu} = r \sqrt{\frac{\mu^{2} - \nu^{2}}{\left( b^{2} - \nu^{2} \right) \left( c^{2} - \nu^{2} \right)}}.

Alternate Definition

An alternative set of conical coordinates have been derived[1]

\begin{align}
\xi   &=  r\cos(\phi\sin\theta)\\
\psi  &=  r\sin(\phi\sin\theta) \\ 
\zeta &=  \theta,
\end{align}

where \{r, \theta, \phi\} are spherical polar coordinates. The corresponding inverse relations are

\begin{align}
r      & =  \sqrt{\xi^2 + \psi^2}\\
\phi   & =  \frac{1}{\sin\zeta}\arctan(\frac{\psi}{\xi}) \\
\theta & =  \zeta.
\end{align}

The infinitesimal Euclidean distance between two points in these coordinates \begin{align}
ds^2  & =  d\xi^2 + d\psi^2+(\xi^2 + \psi^2)(1+\arctan(\frac{\psi}{\xi})^2\cot\zeta^2) d\zeta^2 \\
&+ 2\psi\arctan(\frac{\psi}{\xi})\cot\zeta d\xi d\zeta - 2\xi\arctan(\frac{\psi}{\xi})\cot\zeta d\psi d\zeta.
\end{align}

If the path between any two points is constrained to surface of the cone given by \zeta = \frac{\pi}{4} then the geodesic distance between any two points

\{\xi_1,\psi_1,\zeta_1=\frac{\pi}{4}\} and \{\xi_2,\psi_2,\zeta_2=\frac{\pi}{4}\} is

s^2_{12} = (\xi_1-\xi_2)^2+(\psi_1-\psi_2)^2.

References

  1. Drake, Samuel Picton; Anderson, Brian D. O.; Yu, Changbin (2009-07-20). "Causal association of electromagnetic signals using the Cayley–Menger determinant". Applied Physics Letters 95 (3): 034106. doi:10.1063/1.3180815. ISSN 0003-6951.

Bibliography

External links

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