等离子体组成梯度的热磁不稳定性

J. Sadler, Hui Li
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引用次数: 1

摘要

研究表明,在Braginskii磁流体力学条件下,离子平均电荷态和电子温度的反平行梯度对自生磁场的生长是不稳定的。这种不稳定性类似于产生磁场的热磁不稳定性,尽管它是由碰撞热力磁源项而不是比尔曼电池项驱动的。离子电荷态的梯度引起碰撞的梯度,与温度扰动耦合产生自生磁场。这个磁场以一种强化温度扰动的方式使电子热流偏转。导出的线性化增长率,通常在水动力时间尺度上,包括电阻和热平滑。随着离子组成梯度和电子热流的增大,惯性约束聚变内爆中典型的热腔壁或污染物混合射流的情况下,它会增加。然而,扩展的磁流体动力学模拟表明,与标准的热磁不稳定性类似,非线性能斯特平流通常是不稳定性的主导和稳定因素。
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Thermomagnetic instability of plasma composition gradients
We show that, under Braginskii magneto-hydrodynamics, anti-parallel gradients in average ion charge state and electron temperature can be unstable to the growth of self-generated magnetic fields. The instability is analogous to the field-generating thermomagnetic instability, although it is driven by the collisional thermal force magnetic source term rather than the Biermann battery term. The gradient in ion charge state causes a gradient in collisionality, which couples with temperature perturbations to create a self-generated magnetic field. This magnetic field deflects the electron heat flux in a way that reinforces the temperature perturbation. The derived linearized growth rate, typically on hydrodynamic timescales, includes the resistive and thermal smoothing. It increases with large ion composition gradients and electron heat flux, conditions typical of the hohlraum walls or contaminant mix jets in inertial confinement fusion implosions. However, extended magneto-hydrodynamic simulations indicate that the instability is usually dominated and stabilized by the nonlinear Nernst advection, in a similar manner to the standard thermomagnetic instability.
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