论文标题
等离子体功率平衡在逃亡中的限制
The constraint of plasma power balance on runaway avoidance
论文作者
论文摘要
在缓解或不受限制的速食后血浆中，等离子体功率平衡主要在碰撞或欧姆加热和等离子体辐射冷却之间。在原子混合物的等离子体中，$ \ {n_α\} $与$α$标记原子物种的$α$，功率余额设置了等离子温度，离子电量状态分布$ \ {n_α^i \} $ $ $ i $ $ $ $ $ t_e $ t_e $ t_e $ t_e $ t_e $ t_e $ t_e $ t_e $ t_e $ \ i。 $ e_ \ parallel。$ $以来，由于原子混合物，离子电荷状态分布及其派生的数量及其衍生的数量$ n_e，$ n_e，$ plasma功率在欧欧米克暖气和盘中的限制时，还避免了plase平衡，因此避免了帕斯玛的限制，也是由于原子混合物及其衍生数量$ n_e的原子混合物，离子电荷状态分布及其衍生的数量，也避免了质量范围的机制，也是由原子混合物及其衍生的数量设置的avalanche $ e_ {av} $ $ $。 Tokamak等离子体迅速终止。
In a post-thermal-quench plasma, mitigated or unmitigated, the plasma power balance is mostly between collisional or Ohmic heating and plasma radiative cooling. In a plasma of atomic mixture $\{n_α\}$ with $α$ labeling the atomic species, the power balance sets the plasma temperature, ion charge state distribution $\{n_α^i\}$ with $i$ the charge number, and through the electron temperature $T_e$ and ion charge state distribution $\{n_α^i\},$ the parallel electric field $E_\parallel.$ Since the threshold electric field for runaway avalanche growth $E_{av}$ is also set by the atomic mixture, ion charge state distribution and its derived quantity, the electron density $n_e,$ the plasma power balance between Ohmic heating and radiative cooling imposes a stringent constraint on the plasma regime for avoiding and minimizing runaways when a fusion-grade tokamak plasma is rapidly terminated.
