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Fast-formed liquid surfaces for inertial confinement fusion target shells

机译:用于惯性约束聚变靶壳的快速形成的液体表面

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Advanced ICF targets will have an inner layer of solid or liquid fuel. Their inner surfaces must be smooth and contamination free. All of the current means to produce such a surface have problems: Liquid surfaces sag, solid surfaces tend to facet, and polymer-foam-stabilized surfaces are contaminated by carbon from the foam. An alternative may be to generate a liquid surface immediately before a shot by rapid thermal expansion of a fuel-saturated foam-walled capsule. This approach makes use of the large coefficient of expansion of liquid hydrogen relative to its foam matrix. The shell is filled by exposure to hydrogen vapor during cooling; liquid in the foam has a lower vapor pressure than free liquid, so the shell will fill to exactly 100%. It will stay at that fill fraction as the shell cools and the density of the liquid it contains increases. The shell may be frozen and cooled to 4 K so that it can be stored and handled in vacuum. When the shell is warmed, the liquid expands; the elastic modulus of the foam will force some liquid out of the surface. A simple analysis suggests that a 1 /spl mu/m thick liquid film might be generated in 1 /spl mu/s; that depends on the compressibility of the foam and the flow resistance of its cell structure. Surface tension would smooth this surface layer very rapidly. It would not begin to sag for 1000 /spl mu/s, so there would be sufficient time during which the layer would be satisfactory. An analysis will be presented showing the feasibility of this approach, and the constraints it puts on shell wall structure and insertion-and-shot procedures.
机译:先进的ICF目标将具有固体或液体燃料的内层。它们的内表面必须光滑且无污染。目前生产这种表面的所有方法都存在问题:液体表面下垂,固体表面趋于刻面,聚合物泡沫稳定的表面被泡沫中的碳污染。另一种选择是在即将射击之前通过燃料饱和的泡沫壁胶囊的快速热膨胀产生液体表面。这种方法利用了液态氢相对于其泡沫基质的大膨胀系数。通过在冷却过程中暴露于氢蒸气来填充外壳;泡沫中的液体比自由液体具有较低的蒸气压,因此外壳将完全填充到100%。当外壳冷却并且容纳的液体密度增加时,它将保持在该填充比例。可以将外壳冷冻并冷却至4 K,以便可以在真空中存储和处理外壳。当壳变热时,液体膨胀。泡沫的弹性模量将迫使一些液体流出表面。一个简单的分析表明,可能会以1 / spl mu / s的速度产生1 / spl mu / m的液膜。这取决于泡沫的可压缩性及其泡孔结构的流动阻力。表面张力将非常迅速地使该表面层光滑。它不会在1000 / spl mu / s的时间内开始下垂,因此将有足够的时间使该层令人满意。将进行分析,表明该方法的可行性,以及对壳壁结构和插入-射出程序的限制。

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