Bifurcation in viscoresistive MHD: The Hartmann number and the reversed field pinch

被引:99
作者
Cappello, S
Escande, DF
机构
[1] Consorzio RFX, I-35127 Padua, Italy
[2] CNR, I-00185 Rome, Italy
[3] Univ Aix Marseille 1, UMR 6633 CNRS, F-13397 Marseille, France
关键词
D O I
10.1103/PhysRevLett.85.3838
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A scaling approach to the simplest viscoresistive MI-ID model reveals that the Prandtl number acts only through the inertia term. When this term is negligible the dynamics is ruled by the Hartmann number H only. This occurs for the reversed field pinch dynamics as seen by numerical simulation of the model. When H is large the system is in a multiple helicity state. In the vicinity of H = 2500 the system displays temporal intermittency with laminar phases of quasi-single-helicity (SH) type. For lower H's two basins of SH are shown to coexist. SH regimes are of interest because of their nonchaotic magnetic field.
引用
收藏
页码:3838 / 3841
页数:4
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