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Optimal ion beam, target type and size for accelerator driven systems: Implications to the associated accelerator power

机译:加速器驱动系统的最佳离子束,目标类型和尺寸:对相关加速器功率的影响

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In interactions of different energetic ions with extended targets hydrogen isotopes are the most effective projectiles for the production of spallation neutrons. It is shown that for every target material and incident ion type and energy there is an optimal target size which results in the escape of a maximum number of spallation neutrons from the target. Calculations show that in an ADS, combination of a beam of 1.5 GeV deuteron projectiles and a uranium target results in the highest neutron production rate and therefore highest energy gain. For fast 1.5 GeV d + ~(238)U ADS with lead or lead-bismuth eutectic moderator, the required ion beam current is only 38% of that for 1 GeV proton projectiles on lead target. It is shown that for a modular ADS with uranium target and output power of 550 MW_(th) a 1.5 GeV deuteron beam of current 1.8 mA is required, which is easily achievable with today's technology. For an ADS with K_(eff) 0.98 and output power of 2.2 GW_(th), the required beam currents for (a) 1 GeV p + Pb and (b) 1.5 GeV d + U systems are 18.5 and 7.1 mA, respectively. 【keyworks】Accelerator driven systems;Energy gain;Target types;Optimal target size;ADS power;MCNPX code
机译:在不同的高能离子与扩展目标的相互作用中,氢同位素是产生散裂中子的最有效弹丸。结果表明,对于每种靶材料,入射离子类型和能量,都有一个最佳的靶尺寸,该尺寸可导致从靶中逸出最大数量的散裂中子。计算表明,在ADS中,将1.5 GeV氘核射弹束与铀靶结合使用可获得最高的中子生产率,从而获得最高的能量增益。对于带有铅或铅铋共晶减速剂的1.5 GeV d +〜(238)U ADS的快速ADS,所需的离子束电流仅为铅靶上1 GeV质子弹的离子束电流的38%。结果表明,对于铀靶和输出功率为550 MW_th的模块化ADS,需要电流为1.8 mA的1.5 GeV氘核束,这在当今的技术中很容易实现。对于K_(eff)为0.98,输出功率为2.2 GW_(th)的ADS,(a)1 GeV p + Pb和(b)1.5 GeV d + U系统所需的束电流分别为18.5和7.1 mA。 【主要工作】加速器驱动系统;能量增益;目标类型;最优目标尺寸; ADS功率; MCNPX代码

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  • 来源
    《Annals of nuclear energy》 |2011年第5期|p.1144-1155|共12页
  • 作者单位

    institute of Nuclear Science, School of Physics, A28, University of Sydney, NSW 2006, Australia;

    Institut far Kemchemie, Philipps-UniversitUt, 35032 Marburg, Germany;

    Aristotle University, Thessaloniki, Greece;

    Forschungszentrum Jillich, ISR-6, 52425 Jiilich, Germany;

    Forschungszentrum Jillich, ISR-6, 52425 Jiilich, Germany;

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