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Dynamics of the ballooning mode and the relation to edge-localized modes in a spherical tokamak

机译:球形托卡马克中气球模式的动力学及其与边缘定位模式的关系

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Nonlinear simulations based on the magnetohydrodynamic model have been executed to reveal the dynamics of the ballooning mode in the spherical tokamak plasma. The simulation results have reproduced the characteristic features of the edge-localized mode crash phase, where the filamentary structures are formed along the magnetic field in the edge region, and separated from the core plasma. Moreover, the finite Larmor radius effect is addressed. Nonlinear simulations based on the magnetohydrodynamic model have been executed to reveal the dynamics of the ballooning mode in the spherical tokamak plasma. The simulation results have reproduced the characteristic features of the edge- localized mode crash phase, where the filamentary structures are formed along the magnetic field in the edge region, and separated from the core plasma. Moreover, the finite Larmor radius effect is addressed. (c) 2007 American Institute of Physics.
机译:已经执行了基于磁流体动力学模型的非线性模拟,以揭示球形托卡马克等离子体中的膨胀模式动力学。仿真结果重现了边缘局部模式碰撞阶段的特征,其中沿边缘区域的磁场形成丝状结构,并与核心等离子体分离。此外,解决了有限的拉莫尔半径效应。已经执行了基于磁流体动力学模型的非线性模拟,以揭示球形托卡马克等离子体中的膨胀模式动力学。仿真结果重现了边缘局部模式碰撞阶段的特征,在该阶段,沿边缘区域的磁场形成了丝状结构,并与纤芯等离子体分离。此外,解决了有限的拉莫尔半径效应。 (c)2007年美国物理研究所。

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