真空 ›› 2026, Vol. 63 ›› Issue (2): 27-34.doi: 10.13385/j.cnki.vacuum.2026.02.04
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
LIU Zhipeng1,2, MENG Xiancai2, *, LI Xu2, ZHANG Dehao2, WANG Xiaolong1,2, LIANG Lizhen2,3
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。
中图分类号: TL503.4
| [1] 傅世年,梁天骄,陈和生.BNCT中子源的研发现况与展望[J].科学通报,2022,67(14):1471-1478. [2] NAKAGAWA Y, POOH KH, KOBAYASHI T, et al.Clinical review of the Japanese experience with boron neutron capture therapy and a proposed strategy using epithermal neutron beams[J]. Journal of Neuro-Oncology, 2003, 62: 87-99. [3] KATO I, ONO K, SAKURAI Y, et al.Effectiveness of BNCT for recurrent head and neck malignancies[J]. Applied Radiation and Isotopes, 2004, 61(5): 1069-1073. [4] SUZUKI M.Boron neutron capture therapy (BNCT): a unique role in radiotherapy with a view to entering the accelerator-based BNCT era[J]. International Journal of Clinical Oncology, 2020, 25: 43-50. [5] SAHOO L K, BASAK D, MONDAL A K,et al.The preparation of LiF target for reactions involving 7Li target[J]. Vacuum, 2023, 212: 112055. [6] 王君岩,孔海云,李德明.硼中子俘获治疗中子靶设计[J].核技术,2024,47(4):34-40. [7] 林作康,杨璞,赵乾坤,等.AB-BNCT中子靶物理设计分析[J].原子能科学技术,2020,54(5):804-810. [8] IAEA. Advances in boron neutron capture therapy[R]:Vienna: IAEA, 2023. [9] PHOENIX B,GREEN S,SCOTT M C, et al.Development of a higher power cooling system for lithium targets[J].Applied Radiation and Isotopes, 2015, 106: 49-52. [10] WANG X L, LI J G, WANG J C, et al.Research on the high heat flux removal technique of a lithium target for the AB-BNCT application[J]. Nuclear Engineering and Technology, 2025, 57:103498. [11] HONDA S, YOSHIHASHI S, HAMAJI Y, et al.Evaluation of heat removal performance of a sealed Li target for an accelerator-driven neutron source of boron neutron capture therapy at Nagoya University[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2022, 1042: 167414. [12] HONDA S, YOSHIHASHI S, TOMITA S, et al.Development of a sealed Li target as an accelerator-driven neutron source for boron neutron capture therapy at Nagoya University[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2022, 1040: 167140. [13] QIAO Z P, MA B L, RONG B, et al.Beam shaping assembly design of Li (p, n) neutron source with a rotating target for boron neutron capture therapy[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2023, 1052: 168249. [14] MCMANAMY T, RENNICH M, GALLMEIER F, et al.3 MW solid rotating target design[J]. Journal of Nuclear Materials, 2010, 398(1-3): 35-42. [15] 朱志川. 高热负荷环境下流动液态金属传热行为的流体模拟[D].西南民族大学,2015. [16] 游曦鸣. 液态锂与冷却剂相互作用爆炸特性实验研究[D].上海交通大学,2017. [17] KOBAYASHI T, MIURA K, HAYASHIZAKI N, et al.Development of liquid-lithium film jet-flow for the target of 7Li(p,n)7Be reactions for BNCT[J]. Applied Radiation and Isotopes, 2014, 88: 198-202. [18] KONDO H, KANEMURA T, FURUKAWA T, et al.Validation of IFMIF liquid Li target for IFMIF/EVEDA project[J]. Fusion Engineering and Design, 2015, 96: 117-122. [19] KONDO H, KANEMURA T, PARK C H, et al.Experimental evaluation of wall shear stress in a double contraction nozzle using a water mock-up of a liquid Li target for an intense fusion neutron source[J]. Fusion Engineering and Design, 2019, 146: 285-288. [20] MATSUDA S, KANEMURA T, KONDO H, et al.Measurement of transient flow characteristics of target flow in water experiment for IFMIF[J]. Fusion Engineering and Design, 2017, 124: 1096-1100. [21] NAKAMURA M M,KONDO H,KANEMURA T, et al.Impact of the beam pressure on the free surface of the liquid lithium target of fusion neutron sources[J]. Nuclear Materials and Energy,2018,15:27-31. [22] PAUL M, ARENSHTAM A, HALFON S, et al.A high-power liquid-lithium target (LiLiT) for neutron production[J].Journal of Radioanalytical and Nuclear Chemistry, 2015, 305(3): 783-786. [23] PAUL M, SILVERMAN I, HALFON S, et al.A 50 kW liquid-lithium target for bnct and material-science applications[C]//8th International Meeting of Union for Compact Accelerator-Driven Neutron Sources (UCANS-8). Online: EDP Sciences, 2020:9. [24] 朱志川,张传武,芶富均,等.热通量和液态锂流速对自由流动液态锂温度分布的影响[J].核聚变与等离子体物理,2015,35(2):163-169. [25] BRACKBILL J U, KOTHE D B, ZEMACH C.A continuum method for modeling surface tension[J]. Journal of Computational Physics, 1992, 100(2): 335-354. [26] 李华琪,郭啸宇,杨宁,等.空间堆金属锂冷却剂热物性参数计算模型及程序开发[J].核动力工程,2017,38(1):20-24. [27] 刘永富,谈鹏.液态金属锂在管道中传热特性的数值模拟研究(英文)[J].中国科学技术大学学报,2022,52(1):56-63,72. [28] 卢小龙. 强流离子束包络模拟软件开发及强流中子发生器的物理设计[D].兰州大学,2013. |
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