Title :
Delayed neutron measurement in high frequency mode and its application to the determination of fissile content in spent fuel assembly
Author :
Lee, Tae-Hoon ; Shin, Hee-Sung ; Kim, Ho-Dong
Author_Institution :
Korea Atomic Energy Res. Inst., Daejeon, South Korea
Abstract :
The delayed neutron measurement has been used for the fresh fuel inspection and 235U enrichment measurement of uranium materials for many years. The origin of delayed neutron is the beta decay of fission fragments and the population of fission fragments of right after a fission event decreases as time goes by. In the process of optimization of delayed neutron measurement system using a DT neutron generator to determine the fissile content of spent fuel assembly, we could find out that the utilization of delayed neutron can be maximized by performing the data acquisition of delayed neutron in an earlier time after the fission event. Monte Carlo code simulation results show the delayed neutron count rate obtained in a high frequency mode (100 Hz) is 3.25 times bigger than that acquired in a low frequency mode (0.5 Hz). The influence of delayed neutrons by 238U fission on delayed neutron counts is not negligible. Thus the delayed neutron count rate for 64 cases of spent fuel assembly is corrected by considering the 238U influence. To obtain sufficiently large ratios of signal to background for many cases of spent fuel assembly, 1010 ~ 1011 n/s strength of DT neutron generator is needed.
Keywords :
Monte Carlo methods; beta-decay; fission of uranium; fission reactor fuel; neutron detection; 235U enrichment measurement; 238U fission; DT neutron generator; Monte Carlo code simulation; delayed neutron measurement; fissile content; fission fragment beta decay; fission fragment population; fresh fuel inspection; high frequency mode; spent fuel assembly; Neutrons; Radiation effects;
Conference_Titel :
Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC), 2011 IEEE
Conference_Location :
Valencia
Print_ISBN :
978-1-4673-0118-3
DOI :
10.1109/NSSMIC.2011.6154458