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Multimode short-wavelength perturbation growth studies for the National Ignition Facility double-shell ignition target designs

机译:国家点火设施双壳点火目标设计的多模短波摄动增长研究

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Detailed multimode two-dimensional simulations of short-wavelength perturbations imposed on the material interfaces of a recently proposed indirect-drive double-shell ignition target [Amendt et al., Phys. Plasmas 9, 2221 (2002)] are presented. In this work, the effect of roughness imposed only on the surfaces of the inner shell is studied. Realistic perturbations are adopted from a measured spectrum of a glass capsule (as a surrogate for the high-Z inner shell). It is found that perturbing the inner surface of the inner shell shows minimal degradation in capsule performance. On the other hand, when roughness is imposed on the outer surface of the inner shell, the growth of large Legendre mode number perturbations (l>200) leads to shell breakup. Further analysis reveals a new pathway for the Rayleigh-Taylor (RT) instability. L-shell radiation (>8 keV) from the high-Z hohlraum wall ablates the outer surface of the high-Z inner shell, promoting large outward expansion which is reversed by the converging outer shell. The classic conditions for RT instability are met: low density material pushing onto the higher density inner shell. It is shown that this effect can be controlled by tamping the outward expansion of the inner shell with a variety of materials. Simulations with separate CH and Ti tampers demonstrate that the redesigned capsule can withstand perturbations with high mode number content without exhibiting shell breakup. Furthermore, the outstanding question of determining the cutoff mode number (l(c)) is addressed by performing simulations with successively larger maximum l, reaching values beyond 1000, and calculating the mix width of the pusher/tamper interface for the CH-tamped case. These numerical studies suggest that the mix width approaches a constant value close to 40% of the shell width at peak compression. While not a proof that l(c) has been found, this result suggests that a mix-relevant mode number may be within reach of current simulation capabilities. (C) 2004 American Institute of Physics.
机译:施加在最近提出的间接驱动双壳点火靶材的材料界面上的短波扰动的详细多模二维模拟[Amendt等,Phys。提出了“ Plasmas 9,2221(2002)”。在这项工作中,研究了仅在内壳表面施加粗糙度的影响。从玻璃胶囊的测量光谱中采用实际的摄动(作为高Z内壳的替代物)。发现扰动内壳的内表面在胶囊性能方面显示最小的劣化。另一方面,当对内壳的外表面施加粗糙度时,较大的勒让德模数扰动(l> 200)的增长导致壳破裂。进一步的分析揭示了瑞利泰勒(RT)不稳定性的新途径。来自高Z透孔壁的L壳辐射(> 8 keV)烧蚀了高Z内壳的外表面,从而促进了较大的向外膨胀,该膨胀被会聚的外壳所逆转。满足RT不稳定性的经典条件:将低密度材料推到更高密度的内壳上。结果表明,可以通过用各种材料夯实内壳的向外膨胀来控制这种效果。用单独的CH和Ti篡改进行的仿真表明,重新设计的胶囊可以承受高模数含量的干扰,而不会出现壳破裂的情况。此外,通过执行以下模拟来解决确定截止模式编号(l(c))的悬而未决的问题:依次模拟最大l,达到超过1000的值,并为带有CH的情况计算按钮/篡改接口的混合宽度。这些数值研究表明,在峰压缩时,混合物的宽度接近于壳宽的40%的恒定值。尽管不能证明已找到l(c),但该结果表明与混合相关的模式编号可能在当前的仿真功能范围之内。 (C)2004美国物理研究所。

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