Toroidal coordinates: Difference between revisions
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where ''R<sub>p</sub>'' is the pole of the coordinate system. | where ''R<sub>p</sub>'' is the pole of the coordinate system. | ||
Surfaces of constant ''ζ'' are tori with major radii ''R = R<sub>p</sub>''/tanh ''ζ'' and minor radii ''r = R<sub>p</sub>''/sinh ''ζ''. | Surfaces of constant ''ζ'' are tori with major radii ''R = R<sub>p</sub>''/tanh ''ζ'' and minor radii ''r = R<sub>p</sub>''/sinh ''ζ''. | ||
At ''R = R<sub>p</sub>'', ''ζ'' = | At ''R = R<sub>p</sub>'', ''ζ'' = ∞, while at infinity and at ''R = 0, ζ = 0''. | ||
The coordinate ''η'' is a poloidal angle and runs from 0 to 2π. | The coordinate ''η'' is a poloidal angle and runs from 0 to 2π. | ||
This system is orthogonal. | This system is orthogonal. |
Revision as of 12:20, 13 September 2009
Co-ordinate systems used in toroidal systems:
Cartesian
(X, Y, Z)
Cylindrical
(R, φ, Z), where
- R2 = X2 + Y2, and
- tan φ = Y/X.
φ is called the toroidal angle (and not the cylindrical angle, at least not in the context of magnetic confinement).
Simple toroidal
(r, φ, θ), where
- R = R0 + r cos θ, and
- Z = r sin θ
R0, corresponding to the torus axis, is called the major radius and r the minor radius. θ is called the poloidal angle.
Toroidal
where Rp is the pole of the coordinate system. Surfaces of constant ζ are tori with major radii R = Rp/tanh ζ and minor radii r = Rp/sinh ζ. At R = Rp, ζ = ∞, while at infinity and at R = 0, ζ = 0. The coordinate η is a poloidal angle and runs from 0 to 2π. This system is orthogonal.
Magnetic
See Flux surface.
References
- ↑ Morse and Feshbach, Methods of theoretical physics, McGraw-Hill, New York, 1953 ISBN 007043316X
- ↑ Wikipedia:Toroidal_coordinates
- ↑ F. Alladio, F. Chrisanti, Analysis of MHD equilibria by toroidal multipolar expansions, Nucl. Fusion 26 (1986) 1143