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Magnetic compressibility and ion-temperature-gradient-driven microinstabilities in magnetically confined plasmas

机译:磁压缩性和离子温度梯度驱动   磁约束等离子体中的微观不稳定性

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摘要

The electromagnetic theory of the strongly driven ion-temperature-gradient(ITG) instability in magnetically confined toroidal plasmas is developed.Stabilizing and destabilizing effects are identified, and a critical$\beta_{e}$ (the ratio of the electron to magnetic pressure) for stabilizationof the toroidal branch of the mode is calculated for magnetic equilibriaindependent of the coordinate along the magnetic field. Its scaling is$\beta_{e}\sim L_{Te}/R,$ where $L_{Te}$ is the characteristic electrontemperature gradient length, and $R$ the major radius of the torus. Weconjecture that a fast particle population can cause a similar stabilizationdue to its contribution to the equilibrium pressure gradient. For shearedequilibria, the boundary of marginal stability of the electromagneticcorrection to the electrostatic mode is also given. For a general magneticequilibrium, we find a critical length (for electromagnetic stabilization) ofthe extent of the unfavourable curvature along the magnetic field. This is adecreasing function of the local magnetic shear.
机译:建立了电磁约束环形等离子体中强驱动离子温度梯度(ITG)不稳定性的电磁学理论,确定了稳定和去稳定作用,并确定了临界的\\β_{e} $(电子与磁压之比)为了稳定模式的环形分支,计算了磁平衡,该磁平衡与沿磁场的坐标无关。其缩放比例为$ \ beta_ {e} \ sim L_ {Te} / R,其中$ L_ {Te} $是特征电子温度梯度长度,$ R $是圆环的主半径。我们推测,由于其对平衡压力梯度的贡献,快速的粒子群会引起类似的稳定化。对于剪切平衡,还给出了电磁校正对静电模式的边际稳定性边界。对于一般的磁平衡,我们发现沿磁场的不利曲率程度的临界长度(用于电磁稳定)。这是局部磁剪的递减函数。

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