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ADS功率测量的中子探测技术

Neutron Detection Technique for the Power Measurement in an Accelerator Driven Sub-critical System

  • 摘要: 本工作研究了用于加速器驱动次临界系统(ADS)的堆外中子探测技术。首先,使用FLUKA和OpenMC模拟了ADS系统质子束轰击散裂靶以及次临界反应堆的中子输运过程。根据计算得到的堆外中子能量分布,设计了分别适合于ADS系统高功率量程(HR)和低功率量程(LR)的中子探测系统。压水堆功率量程测量的非补偿涂硼电离室可用于ADS反应堆HR的中子探测,压水堆中间量程测量的γ补偿涂硼电离室可用于ADS反应堆LR的中子探测。此外,针对极低中子注量率的探测,LR的中子探测还可以使用γ补偿的裂变电离室。研究发现,在LR中子探测器前面放置4 cm厚的聚乙烯,可以提高10倍的探测效率。最后,通过Garfield仿真研究了中子探测器的信号处理技术。涂硼电离室和裂变电离室均可使用电流模式的信号处理技术,可探测的中子注量率范围在105~1011 n/(cm2·s)。脉冲模式下裂变电离室还可探测到100 n/(cm2·s)以上的中子注量率。

     

    Abstract: The excore neutron detection technique for the power measurement in an accelerator driven sub-critical system has been studied in this work. Firstly, the physical process of proton beam bombarding spallation target, and the neutron transport process in the subcritical reactor driven in the ADS system have been simulated with FLUKA and OpenMC. Based on the calculated energy distribution of the excore neutrons, the neutron detection systems suit for both the high-power range (HR) and low-power range (LR) in the ADS system have been developed respctively. The uncompensated boron-coated ionization chamber for the power range measurement in pressurized water reactors can be used for the neutron detection of the HR in the ADS system, while the γ-compensated boron-coated ionization chamber for the intermediate range measurement in pressurized water reactors can be used for the neutron detection of the LR in the ADS system. In addition, in order to measure ultra-low neutron fluence rate, the γ-compensated fission chamber can be used for the neutron detection of the LR. It is found in the study that if the polyethylene with a thickness of 4 cm is placed in front of the neutron detectors for the LR, the detection efficiency can increase by 10 times. Finally, the signal processing technology of neutron detectors has been studied through the simulations with Garfield. The signal processing technology of current mode can be used in both the boron-coated ionization chamber and the fission chamber. The detectable neutron fluence rate ranges from 105 to 1011 n/(cm2·s). The fission ionization chamber with the pulse mode can detect neutron fluence rate of 100 n/(cm2·s) or more.

     

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