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LIU Ze-wei, YUE Ai-zhong, LI Bing, ZHAO Jing-yi, JIANG Li-ming, LIU Jiong, MA Hui-sheng, ZHANG Xiao-lei, LU Ning, WANG Shu-sheng. Design and Performance Test of ENT2465 Long-Life Neutron Tube[J]. Journal of Nuclear and Radiochemistry, 2024, 46(2): 131-136. DOI: 10.7538/hhx.2024.YX.2023041
Citation: LIU Ze-wei, YUE Ai-zhong, LI Bing, ZHAO Jing-yi, JIANG Li-ming, LIU Jiong, MA Hui-sheng, ZHANG Xiao-lei, LU Ning, WANG Shu-sheng. Design and Performance Test of ENT2465 Long-Life Neutron Tube[J]. Journal of Nuclear and Radiochemistry, 2024, 46(2): 131-136. DOI: 10.7538/hhx.2024.YX.2023041

Design and Performance Test of ENT2465 Long-Life Neutron Tube

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  • Received Date: April 10, 2023
  • Revised Date: October 07, 2023
  • Available Online: April 22, 2024
  • The neutron tube is the core component of the controllable neutron source logging instrument. Its working stability, temperature resistance, neutron yield and other indicators have an important impact on the working performance of instrument. At present, with the requirement of deep logging, the neutron tube used in logging is supposed to improve neutron yield, temperature resistance, operating life and working stability. In this paper, the structure, materials and manufacturing process of drive-in target neutron tube are designed and optimized to reduce power consumption and improve operating time. The temperature resistance, operating life, and neutron yield of sample tube have tested to estimate the performance of ENT2465 with an outer diameter of 25 millimeters. Place the sample tube in the oil tank of the neutron testing platform and connect the cable. Record the temperature, cumulative working time, neutron yield, target voltage, target current and anode current during the work of the sample tube. The results show that under the target voltage of 80 kV and target current less than 60 μA, the accumulated operating life of the sample tube exceeds 1 000 hours, including 23 hours of continuous operation at 175℃ and more than 500 hours of accumulated operation, and 36 hours of continuous operation at room temperature. The neutron yield only decreases by 5.3 % after 1 000 hours under the same target voltage and current.
  • [1]
    黄隆基.核测井原理[M].东营:石油大学出版社,2000.
    [2]
    杨建峰.测井仪可控式放射源替代伽马源和化学源可行性的分析[C]//中国核学会.2007年中国核学会核技术工业应用分会学术年会,湖北宜昌.2007:67.
    [3]
    谢雨洁.可控源元素测井仪数字化能谱采集电路设计[D].成都:电子科技大学,2022.
    [4]
    万瑞芸,谈效华,肖坤祥,等.潘宁离子源研究概述[J].机电工程技术,2009,38(9):17-19,69,159.
    [5]
    褚庆军,于传武,姜世莲,等.用于孔隙度测井的中子发生器产额影响研究[J].测井技术,2022,46(3):262-267.
    [6]
    谢爱根,裴元吉,孙红兵,等.高能原电子能量与金属的有效真二次电子发射系数的关系[J].强激光与粒子束,2004,16(8):1059-1062.
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