Shafranov shift: Difference between revisions
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The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (1962) 521</ref> is the radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure. | The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (1962) 521</ref> is the outward radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure. | ||
Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta|beta (β)]], and it tends to be more important for [[Tokamak|tokamaks]] than [[Stellarator|stellarators]], | Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta|beta (β)]], and it tends to be more important for [[Tokamak|tokamaks]] than [[Stellarator|stellarators]], | ||
due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case. | due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case. | ||
Revision as of 12:49, 17 August 2010
The Shafranov shift[1] is the outward radial displacement Δ(r) of the centre of flux surfaces with minor radius r, induced by plasma pressure. Typically, the shift is linear [2] in beta (β), and it tends to be more important for tokamaks than stellarators, due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case. [3]
References
- ↑ V.D. Shafranov, At. Energy 13 (1962) 521
- ↑ K. Miyamoto, Plasma Physics and Controlled Nuclear Fusion, Springer-Verlag (2005) ISBN 3540242171
- ↑ T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, Magnetic configuration dependence of the shafranov shift in the Large Helical Device, Plasma Phys. Control. Fusion 48 (2006) 789