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Experimental results of radiation-driven, layered deuterium-tritium implosions with adiabat-shaped drives at the National Ignition Facility

机译:在国家点火设施上用绝热形驱动器进行辐射驱动的氘-layer分层内爆的实验结果

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Radiation-driven, layered deuterium-tritium (DT) implosions were carried out using 3-shock and 4-shock "adiabat-shaped" drives and plastic ablators on the National Ignition Facility (NIF) [E. M. Campbell et al., AIP Conf. Proc. 429, 3 (1998)]. The purpose of these shots was to gain further understanding on the relative performance of the low-foot implosions of the National Ignition Campaign [M. J. Edwards et al., Phys. Plasmas 20, 070501 (2013)] versus the subsequent high-foot implosions [T. Doppner et al., Phys. Rev. Lett. 115, 055001 (2015)]. The neutron yield performance in the experiment with the 4-shock adiabat-shaped drive was improved by factors similar to 3 to similar to 10, compared to five companion low-foot shots despite large low-mode asymmetries of DT fuel, while measured compression was similar to its low-foot companions. This indicated that the dominant degradation source for low-foot implosions was ablation-front instability growth, since adiabat shaping significantly stabilized this growth. For the experiment with the low-power 3-shock adiabat-shaped drive, the DT fuel compression was significantly increased, by similar to 25% to similar to 36%, compared to its companion high-foot implosions. The neutron yield increased by similar to 20%, lower than the increase of similar to 50% estimated from one-dimensional scaling, suggesting the importance of residual instabilities and asymmetries. For the experiment with the high-power, 3-shock adiabat-shaped drive, the DT fuel compression was slightly increased by similar to 14% compared to its companion high-foot experiments. However, the compression was reduced compared to the lower-power 3-shock adiabat-shaped drive, correlated with the increase of hot electrons that hypothetically can be responsible for reduced compression in high-power adiabat-shaped experiments as well as in high-foot experiments. The total neutron yield in the high-power 3-shock adiabat-shaped shot N150416 was 8.5 x 10(15) +/- 0.2 x 10(15), with the fuel areal density of 0.90 +/- 0.07 g/cm(2), corresponding to the ignition threshold factor parameter IFTX (calculated without alpha heating) of 0.34 +/- 0.03 and the yield amplification due to the alpha heating of 2.4 +/- 0.2. The performance parameters were among the highest of all shots on NIF and the closest to ignition at this time, based on the IFTX metric. The follow-up experiments were proposed to continue testing physics hypotheses, to measure implosion reproducibility, and to improve quantitative understanding on present implosion results. Published by AIP Publishing.
机译:辐射驱动的分层氘-((DT)爆炸是在国家点火设施(NIF)上使用3级和4级“绝热形”驱动器和塑料烧蚀器进行的。 M.Campbell等,AIP Conf。进程429,3(1998)]。这些镜头的目的是进一步了解国民点火运动的低脚内爆的相对性能[M. J.Edwards等,《物理学报》。 Plasmas 20,070501(2013)]与随后的高脚内爆[T. Doppner等,Phys。牧师115,055001(2015)]。尽管DT燃料的低模态不对称性较大,但与5个伴随的低脚射击相比,使用4冲击绝热型驱动器的实验中子的屈服性能提高了3到10,与之相似。类似于它的低脚伴侣。这表明低脚内爆的主要降解源是消融前的不稳定性增长,因为绝热体成型显着稳定了这种增长。对于使用低功率3冲击绝热型驱动器的实验,与同伴的高脚内爆相比,DT燃料压缩显着提高了25%到36%。中子产率增加了约20%,低于一维缩放所估计的约50%的增加,表明残余不稳定性和不对称性的重要性。对于使用大功率3冲击绝热型驱动器的实验,与相伴的高脚实验相比,DT燃料压缩略微提高了约14%。但是,与低功率3冲击绝热型驱动相比,压缩率降低了,这与热电子的增加有关,假想可以在大功率绝热型实验以及高足功率实验中降低压缩率实验。高功率3减震绝热形喷枪N150416的总中子产率为8.5 x 10(15)+/- 0.2 x 10(15),燃料面密度为0.90 +/- 0.07 g / cm(2 ),对应着0.34 +/- 0.03的点火阈值因数参数IFTX(在无阿尔法加热的情况下计算),以及因阿尔法加热的2.4 +/- 0.2导致的产量增加。根据IFTX指标,性能参数是NIF上所有镜头中最高的,而此时最接近点火。提出了后续实验,以继续测试物理假设,以测量内爆再现性,并提高对当前内爆结果的定量理解。由AIP Publishing发布。

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