Connection length: Difference between revisions

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In a circular [[tokamak]], the [[Toroidal coordinates|poloidal circumference]] is ''2πr''.
In a circular [[tokamak]], the [[Toroidal coordinates|poloidal circumference]] is ''2πr''.
The connection length is (削除) '' (削除ここまで)L = 2(削除) & (削除ここまで)pi(削除) ; (削除ここまで)r/sin((削除) & (削除ここまで)alpha(削除) ; (削除ここまで))(削除) '' (削除ここまで),
The connection length is (追記) <math> (追記ここまで)L = 2(追記) \ (追記ここまで)pi r/(追記) \ (追記ここまで)sin((追記) \ (追記ここまで)alpha)(追記) </math> (追記ここまで),
where (削除) ''& (削除ここまで)alpha(削除) ;'' (削除ここまで)is the pitch angle of the field line, namely
where (追記) <math>\ (追記ここまで)alpha(追記) </math> (追記ここまで)is the pitch angle of the field line, namely
(削除) '' (削除ここまで)tan((削除) & (削除ここまで)alpha(削除) ; (削除ここまで)) = (削除) B<sub>& (削除ここまで)theta(削除) ;< (削除ここまで)/(削除) sub>/B<sub>& (削除ここまで)phi(削除) ; (削除ここまで)</(削除) sub (削除ここまで)>(削除) '' (削除ここまで).
(追記) <math>\ (追記ここまで)tan((追記) \ (追記ここまで)alpha) = (追記) B_\ (追記ここまで)theta/(追記) B_\ (追記ここまで)phi</(追記) math (追記ここまで)>.
Assuming (削除) ''B (削除ここまで)<(削除) sub (削除ここまで)>(削除) & (削除ここまで)phi(削除) ;</sub> &gt;&gt; B<sub>& (削除ここまで)theta(削除) ; (削除ここまで)</(削除) sub (削除ここまで)>(削除) '' (削除ここまで),
Assuming <(追記) math (追記ここまで)>(追記) B_\ (追記ここまで)phi (追記) \gg B_\ (追記ここまで)theta</(追記) math (追記ここまで)>,
one has (削除) '' (削除ここまで)sin((削除) & (削除ここまで)alpha(削除) ; (削除ここまで)) (削除) &sim; (削除ここまで)tan((削除) & (削除ここまで)alpha(削除) ; (削除ここまで))(削除) '' (削除ここまで), so that
one has (追記) <math>\ (追記ここまで)sin((追記) \ (追記ここまで)alpha) (追記) \simeq \ (追記ここまで)tan((追記) \ (追記ここまで)alpha)(追記) </math> (追記ここまで), so that
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref>
<ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref>


:<math>L = 2 \pi r \frac{B_\phi}{B_\theta} = 2 \pi R q</math>
:<math>L = 2 \pi r \frac{B_\phi}{B_\theta} = 2 \pi R q</math>


where q is the [[Rotational transform|safety factor]], approximated by
where (追記) '' (追記ここまで)q(追記) '' (追記ここまで)is the [[Rotational transform|safety factor]], approximated by
(削除) '' (削除ここまで)q = r (削除) B<sub>& (削除ここまで)phi(削除) ;</sub> (削除ここまで)/ R (削除) B<sub>& (削除ここまで)theta(削除) ; (削除ここまで)</(削除) sub (削除ここまで)>(削除) '' (削除ここまで).
(追記) <math> (追記ここまで)q = r (追記) B_\ (追記ここまで)phi / R (追記) B_\ (追記ここまで)theta</(追記) math (追記ここまで)>.


== Open field lines ==
== Open field lines ==

Revision as of 13:14, 17 April 2015

The connection length is understood to be the distance between two points, measured along a magnetic field line passing through these points.

In the fusion context, a distinction is made between closed field lines (inside the Last Closed Flux Surface) and open field lines (outside).

Closed field lines

In a toroidally confined plasma, inside the Last Closed Flux Surface, the connection length is commonly defined as the length, measured along the magnetic field, to complete a poloidal turn.

In a circular tokamak, the poloidal circumference is 2πr. The connection length is L=2πr/sin(α), where α is the pitch angle of the field line, namely tan(α)=Bθ/Bϕ. Assuming BϕBθ, one has sin(α)tan(α), so that [1]

L=2πrBϕBθ=2πRq

where q is the safety factor, approximated by q=rBϕ/RBθ.

Open field lines

Outside Last Closed Flux Surface, the connection length associated with a given point is defined as the shortest distance from that point to any material surface measured along the field line through that point.

References

  1. K. Miyamoto, Plasma Physics and Controlled Nuclear Fusion, Springer-Verlag (2005) ISBN 3540242171
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