激光聚变在裂变材料生产中的应用

R.N. Horoshko, H. Hurwitz , H. Zmora
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引用次数: 9

摘要

计算了在含有不同浓度238U、239Pu、16O和23Na的介质中,每14MeV中子产生239Pu的量和发生快裂变的次数。中子被认为是由激光诱导的D+T聚变反应产生的,并在钚繁殖的地方与含有肥沃材料的毯子相互作用。计算表明,在纯238U中,中子增殖因子为4.6,每个D+T反应发生1.08次快速裂变。假设En=14MeV下的中子产生率为3×1019秒,并考虑到238U包层的23Na冷却,产生的热能接近1000MW,而产生的239Pu的热值是原来的4倍。在毯子中使用UO2的情况下,数值略低。考虑了239Pu在毯子中的积聚,发现其具有显著增加239Pu净产量和产生的热能的效果。还讨论了在毯子和D+D聚变反应中使用232Th的可能性,发现它们在能量上较差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Application of laser fusion to the production of fissile materials

Calculations are made for the amount of 239Pu produced and the number of fast fissions occuring per 14 MeV neutron in a medium containing various concentrations of 238U, 239Pu, 16O, and 23Na. Neutrons are assumed to be produced by a laser induced D + T fusion reaction and to interact with a blanket containing fertile materials where plutonium breeding occurs. Calculations show that in pure 238U the neutron multiplication factor is 4·6 and that 1·08 fast fissions occur per each D + T reaction. Assuming a neutron production rate of 3 × 1019 sec at En = 14 MeV and allowing for 23Na cooling of the 238U blanket, the thermal energy generated is nearly 1000 MW, while the thermal value of the produced 239Pu is 4 times as large. Values are somewhat lower in cases where UO2 is used in the blanket. Buildup of 239Pu in the blanket is considered and is found to have the effect of strongly increasing both the net 239Pu production and the thermal power generated.

Possibilities of using 232Th in the blanket and the D + D fusion reaction are also discussed and are found to be energetically inferior.

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