DEUTERON INDUCED FUSION REACTION TARGET FOR INERTIAL CONFINEMENT FUSION (ICF)

M. Ibrahim, A. Rimamsiwe, A. Musa,  F A Umar, M. Abdullahi,  F Ahmad, N. F. Isa
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Abstract

 Objective: Energy efficiency enhancement is one of the most effective ways to achieve Fast ignition (FI) in inertial confinement fusion ICF. High energy output gain is essential for ICF reactors and greater energy efficiency can reduce energy costs. The injection of Ion beam is one method used to achieve FI fusion reaction in ICF. A fusion of deuteron with lithium-6 isotope, DLi6 is reviewed in this work alongside the fusion of Deuterium – Tritium (DT), Deuterium – Deuterium (DD), Deuterium – Helium-3 (DHe3) and Proton – Boron-11 (PB11). Materials and Methods: In this work, it is proposed the projection of laser-driven deuteron beam in the FI scheme for ICF in the DLi6 plasma. Fusion occurs as the projected deuteron ion beam hits the lithium-6 target in the thermonuclear fusion reaction. Results: The results show that the fusion reactions of DD, DHe3 and PB11 all require high input kinetic energy (Mega-electronvolts) for the fusion process to occur because of higher Coulomb barrier and the probability of fusion increases by increasing the input energy drive with low output energy gain. DT fusion which require low input kinetic energy of about 400 KeV with high cross section and generated considerable high output energy gain of about 17.59 MeV, However this fusion reaction require large tritium inventory and tritium does not occur naturally, therefore the need for tritium breeding. When the energy of deuteron beam is projected at 200 keV to lithium-6 isotope target, although D + Li6 has a low total cross section of about 19.409 mbarn, the stopping power of the electrons would be more than ions, nuclear stopping power is considerable at very low deuterons energies, the Coulomb interaction of deuteron and lithium-6 occurs with output energy gain of about 22.373 MeV. Conclusion: The investigations indicate that fusion target energy gain efficiency is independent of lithium-6 numerical density. The highest value of energy efficiency gain occurs with lower input kinetic energy of deuteron beam of about 200 KeV to lithium-target. Recommendation: This findings contribute to the core mission of NIF in achieving fast ignition with low ignition energy input to achieve Lawson break-even or "ignition" point of the fusion fuel pellet, where it gives off 100% or more energy than it absorbs. However the simulation results were based on programmed model of Geant4 Hadr03. This results can be validated with the appropriate experimental design of the Hadr03 process.
用于惯性约束聚变(icf)的氘核诱导聚变反应靶
目的:提高能量效率是实现惯性约束聚变ICF快速点火的最有效途径之一。高能量输出增益对ICF反应堆至关重要,更高的能源效率可以降低能源成本。离子束注入是在ICF中实现FI聚变反应的一种方法。本文综述了氘-氚(DT)、氘-氘(DD)、氘-氦-3 (DHe3)和质子-硼-11 (PB11)的核聚变,以及氘与锂-6同位素DLi6的核聚变。材料与方法:本文提出了激光驱动氘核束在DLi6等离子体中用于ICF的FI方案的投影。在热核融合反应中,当投射的氘核离子束击中锂-6目标时,聚变就发生了。结果表明:DD、DHe3和PB11的聚变反应都需要较高的输入动能(兆电子伏)才能发生聚变过程,并且在输出能量增益较低的情况下增加输入能量驱动可以增加聚变的可能性。DT聚变所需的输入动能较低,约为400 KeV,截面高,输出能量增益相当高,约为17.59 MeV,但这种聚变反应需要大量的氚库存,而且氚不是自然产生的,因此需要对氚进行育种。当氘核束能量以200 keV投射到锂-6同位素靶上时,虽然D + Li6的总横截面较低,约为19.409 mbarn,但电子的停止功率大于离子,核在极低的氘核能量下停止功率相当可观,氘核与锂-6发生库仑相互作用,输出能量增益约为22.373 MeV。结论:研究表明,聚变靶能量增益效率与锂-6数值密度无关。当氘核束流对锂靶的输入动能较低,约为200 KeV时,能量效率增益达到最高值。建议:这一发现有助于实现NIF的核心任务,即在低点火能量输入下实现快速点火,以实现Lawson盈亏平衡或聚变燃料颗粒的“点火”点,即它释放的能量超过其吸收的能量的100%或更多。然而,仿真结果是基于Geant4 Hadr03的编程模型。这一结果可以通过适当的Hadr03工艺实验设计来验证。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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