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Reaction Rate Benchmark Experiments with Miniature Fission Chambers at the Slovenian TRIGA Mark II Reactor

机译:斯洛文尼亚赛马标记II反应器的微型裂变室的反应速率基准试验

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A series of fission rate profile measurements with miniature fission chambers, developed by the Commisariat a l'energie atomique et aux energies alternatives, were performed at the Jozef Stefan Institute's TRIGA research reactor. Two types of fission chambers with different fissionable coating (~(235)U and ~(238)U) were used to perform axial fission rate profile measurements at various radial positions and several control rod configurations. The experimental campaign was supported by an extensive set of computations, based on a validated Monte Carlo computational model of the TRIGA reactor. The computing effort included neutron transport calculations to support the planning and design of the experiments as well as calculations to aid the evaluation of experimental and computational uncertainties and major biases. The evaluation of uncertainties was performed by employing various types of sensitivity analyses such as experimental parameter perturbation and core reaction rate gradient calculations. It has been found that the experimental uncertainty of the measurements is sufficiently low, i.e. the total relative fission rate uncertainty being approximately 5 %, in order for the experiments to serve as benchmark experiments for validation of fission rate profiles. The effect of the neutron flux redistribution due to the control rod movement was studied by performing measurements and calculations of fission rates and fission chamber responses in different axial and radial positions at different control rod configurations. It was confirmed that the control rod movement affects the position of the maximum in the axial fission rate distribution, as well as the height of the local maxima. The optimal detector position, in which the redistributions would have minimum effect on its signal, was determined.
机译:由Commisariat A L'Energie Atomique et Aux Energies替代品开发的具有微型裂变室的一系列裂变率曲线测量,在Jozef Stefan Institute的Triga Reseptor Ortor中进行了。使用不同可变性涂层(〜(235)U和〜(238)U)的两种类型的裂变室用于在各种径向位置和几种控制杆配置处执行轴向裂变率曲线测量。基于Triga反应堆的经过验证的蒙特卡罗计算模型,通过广泛的计算集支持了实验活动。计算工作包括中子传输计算,以支持实验的规划和设计以及计算实验和计算不确定性和主要偏见的计算。通过采用各种类型的敏感性分析来进行不确定因素的评估,例如实验参数扰动和核心反应速率梯度计算。已经发现测量的实验性不确定性足够低,即,相对裂变率的总不确定性约为5%,以便实验用作用于验证裂变率分布的基准实验。通过在不同控制杆配置的不同轴向和径向位置的裂变速率和裂变室响应的测量和计算来研究由于控制杆运动引起的中子磁通再分布的影响。确认控制杆运动会影响轴向裂变率分布的最大位置,以及局部最大值的高度。确定了最佳探测器位置,其中重新分配将对其信号产生最小影响。

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