Connection length: Difference between revisions
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== Closed field lines == | == Closed field lines == | ||
In a toroidally confined plasma, inside the [[ | In a toroidally confined plasma, inside the [[Flux surface|Last Closed Flux Surface]], the connection length | ||
is commonly defined as the length, measured along the magnetic field, | is commonly defined as the length, measured along the magnetic field, | ||
to complete a poloidal turn. | to complete a poloidal turn. | ||
In a circular [[ | In a circular [[tokamak]], the [[Toroidal coordinates|poloidal circumference]] is ''2πr''. | ||
The connection length is ''L = 2πr/sin(α)'', | The connection length is ''L = 2πr/sin(α)'', | ||
where ''α'' is the pitch angle of the field line, namely | where ''α'' is the pitch angle of the field line, namely |
Revision as of 16:17, 10 August 2012
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]
where q is the safety factor, approximated by q = r Bφ / R Bθ.
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
- ↑ K. Miyamoto, Plasma Physics and Controlled Nuclear Fusion, Springer-Verlag (2005) ISBN 3540242171