Connection length: Difference between revisions

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Assuming <math>B_\phi \gg B_\theta</math>,
Assuming <math>B_\phi \gg B_\theta</math>,
one has <math>\sin(\alpha) \simeq \tan(\alpha)</math>, so that
one has <math>\sin(\alpha) \simeq \tan(\alpha)</math>, 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>

Latest revision as of 12:36, 26 January 2023

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 Bϕ≫Bθ, 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