首页> 外文会议>The 41st IEEE International Conference on Plasma Science, and the 20th International Conference on High-Power Particle Beams >Vlasov-Fokker-Planck modeling of plasma near hohlraum walls heated with nanosecond laser pulses calculated using the ray tracing equations
【24h】

Vlasov-Fokker-Planck modeling of plasma near hohlraum walls heated with nanosecond laser pulses calculated using the ray tracing equations

机译:使用射线追踪方程计算的纳秒激光脉冲加热的大喇叭口壁附近等离子体的Vlasov-Fokker-Planck建模

获取原文
获取原文并翻译 | 示例

摘要

Summary form only given. Here, we present 2D numerical modeling of near critical density plasma using a fully implicit Vlasov-Fokker-Planck code, IMPACTA, with an implementation of a ray tracing add-on package. This allows to model inverse brehmsstrahlung heating as a laser travels through a plasma by solving the ray tracing equations. In certain situations, such as those at the critical surface at the walls of a hohlraum, magnetic fields are generated through the crossed temperature and electron density gradients (the Biermann Battery effect). Magnetic field generation on the order of MG from the laser heating is shown using a 1 micron laser obliquely incident upon a density ramp. These strong fields along with plasma heating cause the plasma to become strongly magnetized (ωτ > 10). Heat flows are noticeably modified and the temperature profile shows a non-uniformity that does not exist in the case without magnetic fields. The non-uniformities arise because of relatively strong distortions in the distribution function, with different modifications at different spatial points. The distortions in the distribution functions suggest that modification of transport theory may have to be considered for complete understanding of the plasma at hohlraum wall.
机译:仅提供摘要表格。在这里,我们使用完全隐式的Vlasov-Fokker-Planck代码IMPACTA,以及光线跟踪附加组件的实现,对接近临界密度的等离子体进行了2D数值建模。通过解决射线追踪方程,当激光器传播通过等离子体时,这可以模拟反向致冷辐射加热。在某些情况下,例如在大梁壁的关键表面上的那些情况下,磁场是通过交叉的温度和电子密度梯度产生的(比尔曼电池效应)。使用倾斜入射到密度斜坡上的1微米激光显示了从激光加热产生的MG量级的磁场。这些强场以及等离子体加热导致等离子体被强磁化(ωτ> 10)。热流明显改变,温度曲线显示出不均匀性,这种不均匀性在没有磁场的情况下不存在。不均匀性是由于分布函数中相对强烈的失真而引起的,在不同的空间点处进行了不同的修改。分布函数中的失真表明,可能需要考虑对输运理论进行修改,才能完全理解白管壁处的等离子体。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号