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金属学报  2025, Vol. 61 Issue (7): 961-978    DOI: 10.11900/0412.1961.2024.00309
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偏滤器用钨基材料的热负荷损伤行为研究进展
罗来马1,2,3, 陈宇1, 姚刚4, 朱晓勇1,2,3(), 朱大焕5, 吴玉程1,2,3
1 合肥工业大学 材料科学与工程学院 合肥 230009
2 合肥工业大学 高性能铜合金材料及成形加工教育部工程研究中心 合肥 230009
3 合肥工业大学 有色金属与加工技术国家地方联合工程研究中心 合肥 230009
4 内蒙古科技大学 材料科学与工程学院 包头 014010
5 中国科学院合肥物质科学研究院 等离子体物理研究所 合肥 230031
Research Progress on Heat Load Damage Behavior of Tungsten-Based Materials for Divertor
LUO Laima1,2,3, CHEN Yu1, YAO Gang4, ZHU Xiaoyong1,2,3(), ZHU Dahuan5, WU Yucheng1,2,3
1 School of Materials Science and Engineering, Hefei University of Technology, Hefei 230009, China
2 Engineering Research Center of High-Performance Copper Alloy Materials and Processing, Ministry of Education, Hefei University of Technology, Hefei 230009, China
3 National-Local Joint Engineering Research Centre of Nonferrous Metals and Processing Technology, Hefei University of Technology, Hefei 230009, China
4 School of Materials Science and Engineering, Inner Mongolia University of Science and Technology, Baotou 014010, China
5 Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China
引用本文:

罗来马, 陈宇, 姚刚, 朱晓勇, 朱大焕, 吴玉程. 偏滤器用钨基材料的热负荷损伤行为研究进展[J]. 金属学报, 2025, 61(7): 961-978.
Laima LUO, Yu CHEN, Gang YAO, Xiaoyong ZHU, Dahuan ZHU, Yucheng WU. Research Progress on Heat Load Damage Behavior of Tungsten-Based Materials for Divertor[J]. Acta Metall Sin, 2025, 61(7): 961-978.

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摘要: 

有限的能源无法满足人类社会长期发展的需求,核聚变能源被视为保护环境和满足未来能源需求的重要解决方案之一。然而,为确保聚变堆的正常运行,解决托卡马克(Tokamak)装置中面向等离子体的偏滤器热负荷损伤问题至关重要。W因具有高熔点、低物理溅射率、低氘滞留以及优异的力学性能等优点而成为核聚变堆中偏滤器部位首选的面向等离子体材料(PFMs)。在聚变堆运行期间,钨基PFMs会受到持续的热负荷损伤,通常偏滤器部位需承受5~20 MW/m2高热峰值的稳态热负荷和功率密度高达约2 GW/m2的瞬态热负荷。因此,W在热负荷作用下的损伤行为及抑制损伤策略已成为当前研究的热点问题。本文根据国内外现有研究成果,阐述了纯W、合金化钨、弥散强化钨在热负荷作用下的损伤行为。针对钨基材料的热负荷损伤演变情况及抑制损伤策略进行总结与展望,进而为后续研究工作提供参考。

关键词 偏滤器钨基材料热负荷损伤行为抑制损伤策略    
Abstract

Limited energy resources cannot meet the long-term developmental needs of human society. As such, nuclear fusion energy is considered a key solution for environmental protection and meeting future energy demands. However, to ensure the reliable operation of fusion reactors, addressing heat load damage to the divertor facing plasma in tokamak devices is crucial. The divertor, an indispensable core component of fusion devices, plays essential roles in these devices, including the removal of heat load generated via scraping layers and radiation and protection of the main vacuum chamber, auxiliary heating systems, and diagnostic systems, thereby ensuring the safe and stable operation of nuclear fusion reactors. Nevertheless, due to harsh operational conditions, the divertor is prone to damage, limiting the stable operation of long-pulse, high-parameter plasmas. W is critical in the divertor of fusion reactors, primarily owing to its high melting point, low physical sputtering rate, low deuterium retention, and excellent mechanical properties, allowing it to perform stably under extreme conditions. However, tungsten materials have several limitations, including a high ductile-brittle transition temperature, a low recrystallization temperature, and susceptibility to activation. Therefore, it is necessary to regulate, modify, and optimize these materials to enhance the performance of plasma-facing materials (PFMs). Such improvements aim to increase their resilience under extreme environments, minimize damage risks under high heat loads, and enhance heat load resistance, thereby ensuring the long-term stable operation of the divertor in fusion reactors and to meet future energy challenges. The working conditions of fusion reactors are extremely harsh, with the divertor region experiencing continuous heat load damage. It typically faces steady-state heat loads with peak values as high as 5-20 MW/m2 and transient heat loads of up to ~2 GW/m2. These heat loads can cause melting and cracking on both sides of the divertor cassette, posing a risk of reactor failure. Consequently, the study of the heat load damage behavior in tungsten-based PFMs as well as development of damage mitigation strategies have become hot topics in fusion research. This paper reviews current research efforts, both domestic and international, related to the damage behavior of pure tungsten, tungsten alloys, and dispersed phase-strengthened tungsten under heat load conditions. Additionally, it summarizes and forecasts the evolution of heat load damage in tungsten-based materials and presents strategies for damage mitigation, thereby providing a reference for future research endeavors.

Key wordsdivertor    tungsten-based material    heat load    damage behavior    strategies to inhibit the damage
收稿日期: 2024-09-03     
ZTFLH:  TG146.1  
基金资助:国家重点研发计划项目(2019YFE03120002);国家重点研发计划项目(2022YFE03140001);国家重点研发计划项目(2022YFE03030003);中央高校基本科研业务费专项资金项目(JZ2023HGQB0164);国家资助博士后研究人员计划项目(GZC20230656);安徽省自然科学基金项目(2108085J21);安徽省自然科学基金项目(2308085QE154);安徽省重点研发计划项目(202104A05020045)
通讯作者: 朱晓勇,zhuxiaoyong@hfut.edu.cn,主要从事钨基复合材料制备、加工及热负荷研究
作者简介: 罗来马,男,1980年生,教授,博士
图1  磁约束核聚变托卡马克(Tokamak)偏滤器结构设计示意图[2,3]及其热负荷加载场景[13,26]
图2  加载3 GW/m2热负荷后W样品表面的SEM像[27]
图3  主裂纹和二次裂纹典型分布以及不同加载条件下纯W表面开裂情况的SEM像[34]
图4  小型纯W偏滤器模型(SSMU)在高热流测试后的表面形貌[37]
图5  高功率热负荷测试前后再结晶W和电子束选区熔化(SEBM) W的SEM像[39]
Alloy

Grain size

μm

Cracked threshold

GW/m2

Ref.
W020.2< 0.22[51]
W030.3< 0.22[52]
W101< 0.22[51]
W303< 0.22[52]
W100100.44-0.55[51]
表1  超细晶W的抗热负荷能力统计[51,52]
图6  经过氘(D)等离子体暴露热负荷实验后的W和W-3%Ta合金的SEM像[58]
图7  不同高功率密度加载下W-V合金的SEM像[61]
图8  纯W和W-K合金热负荷实验后的SEM像[68]

Alloy

Heat flux

power density

GW·m-2

Behavior

Ref.

W-K-0.05Y0.62Not cracking[71]
W-K-0.10Y0.62Not cracking[71]
W-K-0.25Y0.50Not cracking[71]
W-K-0.50Y0.50Cracking[71]
Deformed pure W0.33Cracking[72]
ITER-reference W> 0.30Cracking[73]
表2  单次热负荷测试中W-K-xY合金和纯W的耐热负荷能力对比[71~73]
图9  热负荷加载后各试样表面的FESEM像[87]
图10  不同功率密度下W-2.0%Y2O3复合材料经100次脉冲热负荷实验后的横向-法向(TD-ND)和轧向-横向(RD-TD)表面形貌[88]
图11  热负荷实验后试样表面和截面的SEM像[92,102]
MaterialApplied surfacePulse numberCracked threshold / (GW·m-2)Ref.
W-0.2%ZrC, rollingRD-TD1000.22-0.33[83]
W-0.5%ZrC, rollingRD-TD1000.22-0.33
W-1.0%TaC, HERF-1000.33-0.44[85]
W-2.0%Y2O3*, rollingRD-TD1000.22-0.33[88]
TD-ND1000.33-0.44
RD-ND100< 0.33[90]
W-0.3%Y2O3, sintering-1> 0.6[92]
W-1.0%La2O3, rollingTD-ND1< 0.22[97]
W-Y2(Ti)O3, SPS-1< 0.30[102]
W-Y2(Mo)O3, SPS-10.60-0.90
W-Y2(Zr)O3, rollingRD–TD1000.3-0.4[103]
W-1.0%La2O3 88%, rolling1> 0.22[106]
W-1.0%TaC, rollingRD–TD1000.33-0.44[107]
W-0.5%TiC, HIPing-100< 0.33[108]
W-1%Y2O3*, HERF-10.55-0.66[109]
W-K-Ti, SPS-100< 0.37[110]
CVD W-11000.28-0.33[111]
Pure W, rollingRD-TD1< 0.22[112]
TD-ND10.22-0.44
RD-TD100< 0.22
表3  经瞬态热负荷后纯W及钨基复合材料损伤行为对比[83,85,88,90,92,97,102,103,106~112]
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