运用FDTD算法对同轴结构的辐照腔不连续性进行了分析,利用CST软件对其进行了结构设计和仿真计算。采用N型射频接头,内外导体采用开孔结构的聚四氟乙烯介质进行支撑,在宽频信号源的激励下,同轴腔内可以产生任意频率和强度的TEM模式的电...运用FDTD算法对同轴结构的辐照腔不连续性进行了分析,利用CST软件对其进行了结构设计和仿真计算。采用N型射频接头,内外导体采用开孔结构的聚四氟乙烯介质进行支撑,在宽频信号源的激励下,同轴腔内可以产生任意频率和强度的TEM模式的电磁场。设计过程中,通过FDTD算法分析与CST软件仿真设计相结合,对超宽频同轴辐照腔的传输性能进行不断优化,在DC^6 GHz频率范围内,S11均在-10 d B以下。展开更多
In the procedure of neutron fluence measurement in the whole energy range (10-4 eV^18 MeV), in the irra- diation chamber of a UZrH reactor, the neutron energy spectra are unfolded using the method of minimizing direct...In the procedure of neutron fluence measurement in the whole energy range (10-4 eV^18 MeV), in the irra- diation chamber of a UZrH reactor, the neutron energy spectra are unfolded using the method of minimizing directed divergence and SAND-II, which are used broadly at home and abroad. These methods belong to the iterative methods. In this article, the procedure of the spectra unfolding using the two methods is described in detail. The neutron spec- trum distribution unfolded by the two methods agree well with each other. In the end, the major differences of the two iterative methods are compared with each other, and the main factors affecting the accuracy of the spectra unfolding with the iterative method are discussed.展开更多
文摘运用FDTD算法对同轴结构的辐照腔不连续性进行了分析,利用CST软件对其进行了结构设计和仿真计算。采用N型射频接头,内外导体采用开孔结构的聚四氟乙烯介质进行支撑,在宽频信号源的激励下,同轴腔内可以产生任意频率和强度的TEM模式的电磁场。设计过程中,通过FDTD算法分析与CST软件仿真设计相结合,对超宽频同轴辐照腔的传输性能进行不断优化,在DC^6 GHz频率范围内,S11均在-10 d B以下。
文摘In the procedure of neutron fluence measurement in the whole energy range (10-4 eV^18 MeV), in the irra- diation chamber of a UZrH reactor, the neutron energy spectra are unfolded using the method of minimizing directed divergence and SAND-II, which are used broadly at home and abroad. These methods belong to the iterative methods. In this article, the procedure of the spectra unfolding using the two methods is described in detail. The neutron spec- trum distribution unfolded by the two methods agree well with each other. In the end, the major differences of the two iterative methods are compared with each other, and the main factors affecting the accuracy of the spectra unfolding with the iterative method are discussed.
