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Effect of hydrogen line radiation on the divertor target plate incident heat flux

机译:氢线辐射对偏滤器靶板入射热通量的影响

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Hydrogen resonance line radiation strongly interacts with the partially ionized plasma at the tokamak edge. As a result of these interactions, a nonlocal plasma energy transport channel opens, altering local atomic level populations by an order-of-magnitude, and affecting plasma transport. Understanding the effects of these interactions is essential to the design of future tokamak divertors, but previous models have not self-consistently treated this physical process. To model the interaction of hydrogen resonance photons with the plasma at the tokamak edge, a partially ionized plasma fluid transport code (PIP) has been developed and integrated into a nonlocal thermodynamics equilibrium (NLTE) code (CRETIN). The partially ionized plasma fluid transport model was derived from kinetic theory and includes the charge-exchange coupling of ions with neutral atoms, transport of internal atomic energy, as well as effective ionization, recombination, and energy loss rates determined by the NLTE model. We apply PIP and CRETIN to the modeling of an optically thick detached tokamak divertor both with and without the effects of line radiation interactions. While many characteristics of the detached divertor regime remain, e.g. the pressure drops in front of the target plate, several details change. Most importantly for the design of future divertors, line radiation interactions increase the divertor target plate incident plasma heat flux from 0.189 MW/m~2 to 0.436 MW/m~2.
机译:氢共振线辐射与托卡马克边缘的部分电离等离子体强烈相互作用。这些相互作用的结果是,一个非局部的等离子能量传输通道打开,从而改变了局部原子能级数量级,并影响了等离子体的传输。理解这些相互作用的影响对于未来托卡马克分流器的设计至关重要,但是以前的模型并不能自洽地对待这一物理过程。为了模拟托卡马克边缘的氢共振光子与等离子体的相互作用,已开发出部分电离的等离子体流体传输代码(PIP),并将其集成到非局部热力学平衡(NLTE)代码(CRETIN)中。部分电离的等离子流体传输模型是从动力学理论推导而来的,包括离子与中性原子的电荷交换耦合,内部原子能的传输以及有效电离,重组和NLTE模型确定的能量损失率。我们将PIP和CRETIN应用于具有和不具有线辐射相互作用影响的光学上较厚的分离托卡马克分流器的建模。分离的分离器制度的许多特征仍然存在,例如在目标板前面的压力下降时,一些细节发生了变化。对于未来分流器的设计最重要的是,线辐射相互作用使分流器目标板的入射等离子体热通量从0.189 MW / m〜2增加到0.436 MW / m〜2。

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