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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Published in: | Journal of the Physical Society of Japan Vol. 70; no. 4; pp. 983 - 987 |
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Main Authors: | , , |
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 |
Subjects: | |
Online Access: | Get full text |
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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. |
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ISSN: | 0031-9015 1347-4073 |
DOI: | 10.1143/JPSJ.70.983 |