Comparison between Double-Resonant and Non-Resonant Mode Driven Convections in a Stellarator with a Non-Monotonic Rotational Transform

For a stellarator (or tokamak) with a non-monotonic rotational transform, both the double-resonant and non-resonant interchange type modes become unstable, when the magnetic curvature is unfavorable in a finite region including the zero magnetic shear surface r=rs. These modes generate convective mo...

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Bibliographic Details
Published in:Journal of the Physical Society of Japan Vol. 70; no. 4; pp. 983 - 987
Main Authors: UNEMURA, Takeshi, HAMAGUCHI, Satoshi, WAKATANI, Masahiro
Format: Journal Article
Language:English
Published: Tokyo Institute of Pure and Applied Physics 01-04-2001
Physical Society of Japan
The Physical Society of Japan
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Summary:For a stellarator (or tokamak) with a non-monotonic rotational transform, both the double-resonant and non-resonant interchange type modes become unstable, when the magnetic curvature is unfavorable in a finite region including the zero magnetic shear surface r=rs. These modes generate convective motions and poloidal shear flows. The non-resonant mode driven convection affects the r [congruent with] rs region significantly, although a decrease of central density is seen. On the other hand, the double-resonant mode driven convection affects the central region for a peaked density profile and a stair-like decrease of the central density is seen. The evolution of the density profile is also correlated with the behavior of the nonlinearly generated poloidal flow.
ISSN:0031-9015
1347-4073
DOI:10.1143/JPSJ.70.983