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Propagation Of Nuclear Data Uncertainties For Fusion Power Measurements

机译:传播核聚变功率测量不确定度

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摘要

Fusion plasmas produce neutrons and by measuring the neutron emission the fusion power can be inferred. Accurate neutron yield measurements are paramount for the safe and efficient operation of fusion experiments and, eventually, fusion power plants. Neutron measurements are an essential part of the diagnostic system at large fusion machines such as JET and ITER. At JET, a system of activation foils provides the absolute calibration for the neutron yield determination.  The activation system uses the property of certain nuclei to emit radiation after being excited by neutron reactions. A sample of suitable nuclei is placed in the neutron flux close to the plasma and after irradiation the induced radiation is measured.  Knowing the neutron activation cross section one can calculate the time-integrated neutron flux at the sample position. To relate the local flux to the total neutron yield, the spatial flux response has to be identified. This describes how the local neutron emission affects the flux at the detector.  The required spatial flux response is commonly determined using neutron transport codes, e.g., MCNP. Nuclear data is used as input both in the calculation of the spatial flux response and when the flux at the irradiation site is inferred. Consequently, high quality nuclear data is essential for the proper determination of the neutron yield and fusion power.  However, uncertainties due to nuclear data are generally not fully taken into account in today’s uncertainty analysis for neutron yield calibrations using activation foils.   In this paper, the neutron yield uncertainty due to nuclear data is investigated using the so-called Total Monte Carlo Method. The work is performed using a detailed MCNP model of JET fusion machine.  In this work the uncertainties due to the cross sections and angular distributions in JET structural materials, as well as the activation cross sections, are analyzed. It is shown that a significant contribution to the neutron yield uncertainty can come from uncertainties in the nuclear data.
机译:聚变等离子体产生中子,通过测量中子发射,可以推断聚变功率。准确的中子产率测量对于聚变实验乃至聚变电厂的安全,有效运行至关重要。在诸如JET和ITER的大型聚变机器上,中子测量是诊断系统必不可少的部分。在JET,活化箔系统为中子产率测定提供了绝对校准。活化系统利用某些原子核的特性在被中子反应激发后发出辐射。将合适的核样品放置在靠近等离子体的中子通量中,并在辐照后测量诱发的辐射。知道中子活化截面,就可以计算出样品位置处的时间积分中子通量。为了将局部通量与总中子产率相关联,必须确定空间通量响应。这描述了本地中子发射如何影响检测器处的​​通量。通常使用中子传输码例如MCNP来确定所需的空间通量响应。在空间通量响应的计算中以及在推断辐照部位的通量时,都将核数据用作输入。因此,高质量的核数据对于正确确定中子产率和聚变能力至关重要。但是,在当今使用活化箔进行中子产率校准的不确定性分析中,通常不会完全考虑到核数据带来的不确定性。在本文中,使用所谓的总蒙特卡罗方法研究了由于核数据而引起的中子产率不确定性。使用详细的JET融合机MCNP模型进行工作。在这项工作中,分析了由于JET结构材料的横截面和角度分布以及激活横截面引起的不确定性。结果表明,对中子产率不确定性的重要贡献可能来自核数据的不确定性。

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