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真空 ›› 2026, Vol. 63 ›› Issue (2): 27-34.doi: 10.13385/j.cnki.vacuum.2026.02.04

• 真空应用 • 上一篇    下一篇

基于BNCT的耐高热负荷液态锂靶设计*

刘志鹏1,2, 孟献才2, 李旭2, 张德皓2, 王小龙1,2, 梁立振2,3   

  1. 1.安徽理工大学 机电工程学院,安徽 淮南 232001;
    2.合肥综合性国家科学中心能源研究院(安徽省能源实验室),安徽 合肥 230031;
    3.中国科学院合肥物质科学院等离子体物理研究所,安徽 合肥 230031
  • 收稿日期:2025-06-16 出版日期:2026-03-25 发布日期:2026-03-27
  • 通讯作者: 孟献才,副研究员,硕导。
  • 作者简介:刘志鹏(2002-),男,安徽阜阳人,硕士研究生。
  • 基金资助:
    *国家重点研发计划项目(2024YFE03250600,2024YFE03000200); 安徽省自然科学基金项目(2308085MA22); 国家自然科学基金青年项目(12305200); 合肥综合性国家科学中心能源研究院(安徽省能源实验室)项目(21KZS202)

Design of a Liquid Lithium Target Resistant to High Heat Load for BNCT

LIU Zhipeng1,2, MENG Xiancai2, *, LI Xu2, ZHANG Dehao2, WANG Xiaolong1,2, LIANG Lizhen2,3   

  1. 1. School of Mechanical and Electrical Engineering, Anhui University of Science and Technology, Huainan 232001, China;
    2. Institute of Energy, Hefei Comprehensive National Science Center (Anhui Energy Laboratory), Hefei 230031, China;
    3. Institute of Plasma Physics, Chinese Academy of Sciences, Hefei, 230031, China
  • Received:2025-06-16 Online:2026-03-25 Published:2026-03-27

摘要: 加速器硼中子俘获治疗装置中通常采用锂靶作为中子靶,但高热负荷沉积会缩短靶寿命,因此耐高热负荷的靶是维持装置稳定运行的关键。本文设计了一种在真空环境下耐30 MW/m2以上高热负荷的液态锂靶模块,可以在承受50 kW高能质子的轰击时将液态锂的温度控制在600 K安全阈值内。该液态锂靶模块主要由喷嘴、凹形背板、收集槽和加热丝等部分组成。文章重点模拟了液态锂模块的喷嘴宽度、液态锂流速和凹形背板半径三个因素对高热负荷移除能力的影响。结果表明喷嘴宽度从1.5 mm增加至3 mm时液态锂膜的厚度从1.2 mm增加至2.3 mm,进而使液态锂表面最高温升从82 K降至52 K,后续增加喷嘴宽度并无明显变化。液态锂流速从7 m/s增加至14 m/s,其温升从91 K降至46 K,但温升之间的差值逐渐减小。凹形背板半径从500 mm减至250 mm时,液态锂最高温升从77 K降至43 K,且对比直板结构,能够有效提高锂膜的均匀性和稳定性。该研究结果可以为液态锂靶的工程实践提供一定的参考,为硼中子俘获治疗的稳定运行提供了一种可行的办法。

关键词: 液态锂靶, 热负荷, 中子源, 硼中子俘获治疗

Abstract: In accelerator-based boron neutron capture therapy (BNCT) device, the Li target is commonly employed for neutron production. However, the lifetime of Li target is significantly reduced due to the high heat load deposition. Consequently, the target capable of withstanding high heat load is critical for ensuring stable operation of BNCT device. A liquid Li target module which is capable of withstanding heat fluxes exceeding 30 MW/m² in vacuum environment is designed in this paper. The module can maintain the liquid Li temperature below the safe threshold of 600 K even under irradiation by a 50 kW high-energy proton beam. The key components of the liquid Li target module include a nozzle, a concave back plate, a collection tank and heating wire. The effect of nozzle width, Li flow rate, and concave back-plate radius on the high-heat-flux removal capability of the module were simulated. The results demonstrate that, with liquid Li film thickness increasing from 1.2 mm to 2.3 mm as nozzle width increases from 1.5 mm to 3.0 mm, the surface temperature rise decreases from 82 K to 52 K. Furthermore, no significant further improvement in the heat removal capability of the target is observed when the nozzle width is increased beyond 3.0 mm. While increasing the liquid Li flow rate from 7 m/s to 14 m/s reduces the maximum temperature rise from 91 K to 46 K, the reduction in temperature rise gradually diminishes. When decreasing the concave back-plate radius from 500 mm to 250 mm, the maximum temperature rise of liquid Li decreases from 77 K to 43 K. Compared to a flat-plate structure, the concave design can effectively improve the uniformity and stability of the Li film. These findings provide valuable guidance for the engineering implementation of liquid Li targets and offer a feasible approach for ensuring stable operation of boron neutron capture therapy systems.

Key words: liquid Li target, heat load, neutron source, boron neutron capture therapy

中图分类号:  TL503.4

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