金属学报, 2023, 59(4): 513-522 DOI: 10.11900/0412.1961.2023.00123

综述

表面状态对核电关键材料腐蚀和应力腐蚀的影响

韩恩厚,1,2,3, 王俭秋1

1中国科学院金属研究所 中国科学院核用材料与安全评价重点实验室 沈阳 110016

2广东腐蚀科学与技术创新研究院 广州 510535

3华南理工大学 材料科学与工程学院 广州 511442

Effect of Surface State on Corrosion and Stress Corrosion for Nuclear Materials

HAN En-Hou,1,2,3, WANG Jianqiu1

1CAS Key Laboratory of Nuclear Materials and Safety Assessment, Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China

2Institute of Corrosion Science and Technology, Guangzhou 510535, China

3School of Materials Science and Engineering, South China University of Technology, Guangzhou 511442, China

通讯作者: 韩恩厚,ehhan@scut.edu.cn,主要从事材料腐蚀机理、腐蚀控制技术、装备服役安全评定技术研究与工程应用

责任编辑: 肖素红

收稿日期: 2023-03-24  

基金资助: 国家重点基础研究发展计划项目(2011CB610500)
国家重点基础研究发展计划项目(2006CB610500)
国家重大科技专项项目(2011ZX06004-009)
国家重点研发计划项目(2016YFE0105200)
中国科学院重点部署项目(ZDRW-CN-2017-1)
中国科学院前沿科学重点研究计划项目(QYZDY-SSW-JSC012)

Corresponding authors: HAN En-Hou, professor, Tel:(020)22309460, E-mail:ehhan@scut.edu.cn

Received: 2023-03-24  

Fund supported: National Basic Research Program of China(2011CB610500)
National Basic Research Program of China(2006CB610500)
National Science and Technology Major Project of China(2011ZX06004-009)
National Key Research and Development Program of China(2016YFE0105200)
Key Programs of Chinese Academy of Sciences(ZDRW-CN-2017-1)
Key Research Program of Frontier Sciences, Chinese Academy of Sciences(QYZDY-SSW-JSC012)

作者简介 About authors

韩恩厚,男,1961年生,教授,博士

摘要

全球迄今发生的核电安全事件往往是由局部腐蚀造成,而局部腐蚀从表面起始。表面状态如何影响腐蚀,以及辐照和应力与之的交互作用已经成为核电站运行安全性、可靠性、经济性保障的重要技术难题之一。本文系统总结了在过去十余年的国家系列项目支持下,针对核电用关键结构材料在不同表面加工与划伤后微观组织变化、在模拟核电站一回路水中的腐蚀、应力腐蚀和辐照促进应力腐蚀行为,并将这些腐蚀行为与材料的微观组织以及力学、辐照等多因素相关联。结果表明,打磨、划伤和切削加工都会使材料近表面产生不同程度的梯度结构,表面变形层状态存在较大差异。划伤后,在划伤底部存在大于屈服极限的残余压应力。相同粗糙度的切削加工表面,机加工参数不同可以导致深度方向上形成的纳米晶区、晶粒畸变区梯度结构明显不同。这种微观组织与局部应力应变条件使得材料抗腐蚀能力差异显著,例如划伤导致的应力腐蚀裂纹数量与划伤深度正相关。在辐照、腐蚀、应力的联合作用下,辐照促进应力腐蚀敏感性进一步升高。最后展望了未来发展趋势。

关键词: 表面状态; 腐蚀; 应力腐蚀; 辐照促进应力腐蚀; 核电材料; 不锈钢; 镍基合金

Abstract

Global nuclear power events are often caused by local corrosion, which starts at the surface. The effect of the surface state on corrosion and the interaction among corrosion, irradiation, and stress are important technical problems affecting the safety, reliability, and economy of nuclear power plants. In this paper, supported by a series of national projects in the last 10 years, the various surface state effects, for key structural materials used in nuclear power plants after surface finishing, grinding, machining, or scratching, on corrosion and stress corrosion behaviors in the simulated primary water of nuclear power plants are reviewed. The results show that surface grinding, scratching, or cutting can cause the formation of microstructures of different gradients near the surface and also cause large differences in surface deformation. For example, the residual compressive stress is greater than the yield stress in the superficial surface of the scratch; the different cutting parameters can cause the various gradient structures of the nanocrystalline and grain distortion zones to form along the depth of the cutting surface with similar surface roughness. Such microstructures and local stress-strain conditions lead to significant differences in corrosion resistance. For example, the number of stress corrosion cracks is positively correlated with scratch depth. Under the combined action of irradiation, corrosion, and stress, irradiation-assisted stress corrosion is further enhanced. Finally, the future research trend on the topic is forecast.

Keywords: surface state; corrosion; stress corrosion; irradiation-assisted stress corrosion; nuclear material; stainless steel; nickel-based alloy

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本文引用格式

韩恩厚, 王俭秋. 表面状态对核电关键材料腐蚀和应力腐蚀的影响[J]. 金属学报, 2023, 59(4): 513-522 DOI:10.11900/0412.1961.2023.00123

HAN En-Hou, WANG Jianqiu. Effect of Surface State on Corrosion and Stress Corrosion for Nuclear Materials[J]. Acta Metallurgica Sinica, 2023, 59(4): 513-522 DOI:10.11900/0412.1961.2023.00123

核能利用以来出现的核电安全事件的统计结果表明,腐蚀是影响核电站安全性、可靠性、经济性的第一要素[1~4]。仅一回路水接触的核电设备面积约2 × 104 m2。表面质量直接影响腐蚀速率和放射性废物的排出量。材料的均匀腐蚀从设计时已经考虑,通过不断提高水化学控制技术水平,可以进一步降低腐蚀速率和放射性废物量的排出。统计表明,全球迄今发生的核电事件往往是由局部腐蚀造成[2]。传统上,研究局部腐蚀大多关注损伤后期的扩展,例如应力腐蚀裂纹扩展、腐蚀疲劳裂纹扩展、点蚀坑的深度扩展等。裂纹萌生与点蚀坑萌生研究得非常不充分,这主要是由于早期的腐蚀损伤尺寸小、速率低,研究手段受限[3,4]。从工程角度看,无论是美国、欧洲还是我国,核电装备设计与制造标准中通常以表面光洁度来控制表面质量。而实际核电站中的腐蚀案例表明,腐蚀的发生与发展都是从设备表面开始的,表面存在宏观缺陷部位(例如划伤)的起始扩展通常容易理解,但看似同样的光滑表面在运行中出现腐蚀损伤的时间存在巨大差别,对此一直难以给出合理解释。由此可见,设备或材料的表面状态复杂,例如表层的微观组织、残余应力与残余应变、腐蚀性环境因子与应力、辐照与材料微观特征的交互作用等存在很大的不确定性。然而,国际上开展的相关实验研究尚不充分,尤其是一直缺乏深入系统的机理研究,致使核电装备制备工艺难以得到有效优化,已经成为核电站运行安全性、可靠性、经济性保障的重要技术难题之一[5,6]

本文综述了在过去十余年国家系列项目支持下,针对核电用关键结构材料,如镍基合金690和600、不锈钢304和316以及焊材182等,通过比较机械打磨、机械抛光、电解抛光、不同机械加工切削工艺以及表面划伤后样品在模拟核电站一回路水中的腐蚀、应力腐蚀开裂(SCC)和辐照促进应力腐蚀开裂(IASCC)等方面的研究结果,特别是把这些腐蚀行为与材料的微观组织以及力学状态相关联,在澄清机理的基础上为优化核电装备制造工艺和提升标准奠定技术基础。

1 不同表面状态核电材料的微观组织

1.1 打磨、机械抛光、电解抛光对690镍基合金的影响

采用商用690镍基合金传热管的外径为19 mm,壁厚为1.09 mm。材料主要化学成分(质量分数,%)为:Cr 29.02,Fe 10.28,Mn 0.30,Ti 0.33,S 0.001,P 0.009,C 0.018,N 0.0234,Si 0.31,Cu 0.010,Co 0.015,Al 0.16,Ni余量。材料的最终热处理工艺为:1050℃下固溶处理0.5 h,水冷;然后在715℃下保温15 h (TT处理)。690TT合金的晶粒尺寸为20~50 μm,有大量孪晶和少量TiN析出相,在晶界处分布有近连续或半连续的Cr的碳化物[7~14]

690TT合金管材样品分别经过400号砂纸打磨、1500号砂纸打磨、机械抛光和电解抛光4种表面处理。打磨至400号的样品表面粗糙度最大,电解抛光的样品表面粗糙度最低。然后对4种样品的近表面截面的微观组织进行透射电镜(TEM)观察。图1[11]是4种表面状态样品的截面TEM像,发现在近表面存在表面变形层,并且变形层厚度随表面处理条件不同发生变化,从400号打磨样品变形层厚度为470 nm、1500号打磨样品变形层厚度为285 nm、机械抛光样品变形层厚度为140 nm、直到电解抛光没有观察到变形层。由于690TT合金的层错能很低,打磨处理能够使样品近表面微观上发生位错运动,且容易形成机械孪晶和宏观上发生塑性变形,这种冷加工的引入使得变形层发生晶粒细化直至形成纳米结构。随着使用打磨的砂纸粒度降低,应变程度也降低,导致变形层厚度和晶粒细化程度也在逐渐降低。

图1

图1   不同表面状态690TT合金冷加工影响层截面的TEM像和选区电子衍射花样[11]

Fig.1   Cross-section TEM images and SAED patters (insets) of alloy 690TT samples with different surface states

(a) ground to 400 grit (b) ground to 1500 grit

(c) mechanically polished (d) electropolished


1.2 划伤后690TT合金表面的微观结构与残余应力

由于制作工序,在装配过程中,蒸汽发生器传热管、燃料包壳管等不可避免地会产生表面划伤。在实验室模拟制备了与现场管材尺寸相近的划伤,并对划伤后的材料进行了组织结构观察和残余应力测量。690TT合金划伤两侧的晶粒出现了严重的塑性变形并产生了大量的滑移台阶[15]。因划伤过程,划伤沟槽底部晶界出现弯曲(图2a[16]),划伤沟槽底部的微观组织TEM观察发现,从划伤沟槽中心到划伤两侧出现了纳米晶(图2b[16])和机械孪晶的梯度变形结构(图2c[16]),这与表面打磨后出现细晶层(图1[11])的现象一致,只是划伤过程中材料的塑性应变速率高,细晶层厚度更大。

图2

图2   690TT合金表面划伤的截面[16]

Fig.2   Cross-section of the scratch in alloy 690TT[16]

(a) SEM observation

(b) TEM observation of the nano-grains at the bottom of the scratch

(c) TEM observation of the mechanical twins at the bank of the scratch


利用同步辐射硬X射线对划伤浅表面组织中存在的残余应力进行了测量[17],结果显示浅表面(20 μm)的残余压应力为(414 ± 29) MPa,沿划伤沟槽方向的残余拉应力为(467 ± 15) MPa,远远超过690TT合金的屈服强度(303 MPa)。

1.3 切削加工对304不锈钢表层微观组织的影响

切削加工是一种广泛使用的减材制造技术,通常人们关注的是加工后的表面光洁度。事实上,切削加工会引起材料发生剧烈塑性变形,甚至使材料表面纳米化,进而使材料表面的电化学腐蚀行为发生明显改变。采用7种不同工艺参数对国产核用304不锈钢(主要化学成分(质量分数,%)为:C 0.053,Cr 18.45,Ni 8.3,N 0.057,Mn 1.59,Si 0.47,S 0.004,P 0.022,Fe余量;1050℃下保温30 min,随即进行淬火处理)表面进行切削加工,切削加工使样品近表面发生变形,加工参数的影响明显并具有规律性。通过电子背散衍射(EBSD)分析(图3[18]),结果表明,材料在切削过程中发生了严重的塑性变形,存在大量剪切变形带。核平均取向错位(KAM)图中近表面表现出很高的残余应变,当切削深度和切削速率保持一致时,大进给量会产生更大的加工影响区域(MAZ);当进给量和切削深度保持一致时,低切削速率会产生更大的MAZ;而当切削速率和进给量保持一致时,小切削深度会产生更大的MAZ。KAM观察与截面硬度测量结果相一致。

图3

图3   7种切削加工工艺的核用304不锈钢样品近表面截面的EBSD分析[18]

Fig.3   EBSD analyses of cross-sectional deformation of the machined samples (Samples from #1 to #7 are arranged in order from left to right)[18]

(a) band contrast (BC) map (b) inverse pole figure (IPF) (c) kernel average misorientation (KAM) map


奥氏体不锈钢塑性变形过程主要由位错运动、孪生变形完成。由于切削过程中力和热的综合作用,材料近表面发生严重塑性变形。对进给量0.20 mm/r、切削速率450 r/min、切削深度1 mm的样品近表面观察发现,在表层几个微米范围内应变大,同时刀具与工件表面摩擦产生的热效应明显,晶粒发生纳米化;在近表面纳米晶区以下5~300 μm塑性变形主要为位错运动,位错沿着特定的滑移系运动,形成与切削表面呈特定角度的夹角,具有孪晶结构的变形带。因此,经过切削加工后,材料在深度方向上形成了纳米晶区、晶粒畸变区、基体的梯度结构[19]

2 表面状态对核电材料腐蚀行为的影响

表面加工工艺或表面划伤会使材料表面产生塑性变形,变形后滑移台阶位置的电化学活度比未滑移区域要高,故而会加速材料腐蚀的发生与发展。

2.1 抛光工艺对核电结构材料在高温高压水中腐蚀行为的影响

作者团队[20~26]系统研究了机械抛光和电解抛光以及表面状态对核用316L不锈钢、600镍基合金、182镍基焊材以及308L不锈钢焊材的腐蚀行为影响。以核用316L不锈钢为例,其主要化学成分(质量分数,%)为:Cr 16.3,Ni 12.9,Mo 2.2,Mn 0.7,Si 0.51,C 0.014,P 0.028,S 0.0017,Fe余量。分别进行电解抛光和 SiO2机械抛光后,对比其在核电高温高压水中的腐蚀行为[19]。316L不锈钢电解抛光表面在核电高温高压水中生成的腐蚀产物膜厚度大于SiO2机械抛光表面(图4[20]),电解抛光表面的抗腐蚀能力要比SiO2机械抛光表面的差[19]。事实上,在腐蚀早期这种差异更加明显。产生这种差异的原因主要是电解抛光表面初始膜的氢氧化物含量较高,其保护性差且会促使阴/阳离子在氧化物中的扩散。在腐蚀后期,氢氧化物逐渐转变为氧化物,其作用逐渐减弱,2种抛光表面的腐蚀速率逐渐接近。事实上,这种腐蚀速率的变化来自材料表面的H、O、OH-、H2O与Cl-等的吸附及其与材料或表面尖晶石腐蚀产物之间的交互作用[27~34]

图4

图4   电解抛光和SiO2机械抛光316L不锈钢样品在核电一回路高温高压水中腐蚀500 h后氧化膜的TEM分析[20]

Fig.4   TEM observations and analyses of the oxide scale formed on electropolished surface (EPS) (a, c) and colloidal silica slurry polished surface (CPS) (b, d) on 316L following the 500 h exposure in high temperature water[20]

(a, b) TEM images and corresponding SAED patterns (insets) showing the cross-section of the oxide scale and the area analyzed (c, d) EDS mappings for O, Ni, Cr, and Fe, respectively


2.2 切削加工304不锈钢在高温水中的腐蚀行为[18,19]

把不同参数切削加工后的国产核用304不锈钢样品在模拟核电一回路水溶液中(1500 × 10-6 B (H3BO3),2.3 × 10-6 Li (LiOH·H2O),溶解氢含量2.6 × 10-6 (30 cm3 H2/(kg H2O)),温度为340℃,压力16 MPa)进行腐蚀实验720 h后发现,样品表面生长着细小的颗粒状氧化物,外层氧化物颗粒具有Fe3O4尖晶石结构;内层氧化膜是很薄的富Cr层。表层整体的氧化膜厚度约7.5 nm,腐蚀速率较低。

在距离切削加工表面约50 μm处晶粒畸变区腐蚀后的截面可以观察到大量的变形带以及沿变形带和晶界发生了择优腐蚀。对晶粒畸变区择优腐蚀的晶界和变形带进行的TEM形貌、结构及成分分析发现,在晶界上沿晶腐蚀的长度有近200 nm;在沿晶腐蚀前沿有纳米尺度的氧化物且有明显的Ni富集,Ni富集的长度近200 nm。通过选区电子衍射发现机加工影响区内的变形带具有孪晶结构(图5a[18]),沿变形带发生的择优腐蚀长度超过600 nm (图5b[18]),变形带发生的择优腐蚀速率远大于沿晶腐蚀。变形孪晶腐蚀产物与基体界面处轻微富Cr并且腐蚀产物前沿有轻微富Ni (图5cd[18])。

图5

图5   核用304不锈钢切削加工影响区内变形带腐蚀的TEM形貌[18]

Fig.5   TEM bright-field corrosion morphology at the deformed zone of sample #5, with the inserted SAED pattern (a); high-angle annular dark field (HAADF) image of the deformation twin corrosion area (b); EDS mapping analyses of Cr, Fe, Ni, and O elements (c); EDS line scan analyses across the corroded deformation twin (d) (Under scanning transmission mode, the electron beam spot size is 1.5 nm, and the scanning step size is 2 nm)[18]


3 表面划伤对应力腐蚀行为的影响

应力腐蚀裂纹通常沿着与拉应力垂直的方向扩展。通过对690TT镍基合金在高温含Pb浓碱溶液中的实验发现,划伤诱发的应力腐蚀裂纹与残余拉应力的方向相同(图6[35])。划伤诱发的应力腐蚀裂纹可以在划伤沟槽的宏观压应力区产生,氧化物生长时产生的楔形力是在该区域裂纹萌生和扩展的驱动力,而不是传统概念中与划伤沟槽方向一致的残余拉应力[15~17,35~40]。划伤变形造成了划伤周围的能量分布不同,特别是划伤沟槽浅表面的纳米晶储存了较高的变形能,这种高能区优先发生氧化和溶解,最终导致腐蚀裂纹萌生。

图6

图6   应力腐蚀裂纹沿划伤沟槽晶界、滑移台阶生长[35]

Fig.6   Stress corrosion carcking (SCC) cracks growth[35]

(a) transgranular stress corrosion carcking (TGSCC) underneath a scratch

(b) intergranular stress corrosion carcking (IGSCC) at scratch bank


4 表面状态、腐蚀、辐照、应力的交互作用

辐照使晶格上的原子离开其初始位置而形成空位、间隙原子以及嬗变等缺陷,在一定温度下,碰撞产生的空位和间隙原子在晶格中扩散,可聚集成空位团或形成位错环。一些元素在晶界和位错环处发生元素偏析,并引起材料硬度的增加。位错环平均尺寸和数量密度、晶界偏析程度以及辐照硬化程度均随辐照剂量增加而增加[41]。事实上,核电材料的辐照损伤程度与材料的表面状态、腐蚀条件、应力水平密切相关[42~45]。腐蚀与裂纹往往从表面缺陷处萌生,这些缺陷包括夹杂物、表面元素分布不均匀、应力分布不均匀等。在辐照、腐蚀、应力的联合作用下,晶粒内部产生滑移台阶,并在该位置优先产生腐蚀或萌生裂纹。通过不同辐照剂量(0.5、1.5、3和5 dpa)、不同应变(0、3%)的核级304不锈钢样品在核电高温高压水中的实验发现[46],辐照可促进表面滑移台阶和晶界处局部变形,且晶界和滑移台阶处残余应变集中程度随辐照剂量增加而增加;在应变作用下晶界腐蚀速率明显高于无应变作用下的晶界腐蚀速率;表面滑移台阶处局部腐蚀氧化物深度随台阶高度增加而增加(图7a[46]);增加辐照剂量可促进核用304不锈钢在压水堆一回路水中的IASCC敏感性(图7b[46])。

图7

图7   核级304不锈钢无应变与3%应变样品的沿晶氧化与辐照剂量的关系;辐照促进应力腐蚀开裂的敏感性(裂纹数量与长度)与辐照剂量的关系[46]

Fig.7   Depth of intergranular oxide in strain-free and 3% strained specimens as a function of irradiation dose (PWR—pressurized water reactor, DH—dissolved hydrogen) (a), irradiation-assisted stress corrosion cracking (IASCC) susceptibility as measured by crack number and crack length per unit area as a function of irradiation dose (b)[46]


5 结论与展望

系统总结了过去十余年来有关材料表面状态如何影响核用结构材料的微观组织与在模拟核电站一回路高温高压水中腐蚀行为方面的研究结果,结论如下:

(1) 不同表面加工手段,材料近表面的局部特征存在显著差异。机械打磨、机械抛光等不仅使材料近表面微观结构表现出梯度变化,特别是表面变形层存在较大差异,变形层的厚度和微观结构由进行表面处理时的局部应变幅和应变速率决定。表面划伤后,划伤底部存在大于屈服极限的残余压应力,沿划伤沟槽方向则存在大于屈服极限的残余拉应力。切削加工的材料近表面区域,在深度方向上形成了纳米晶区、晶粒畸变区、基体的梯度结构。粗糙度相同的情况下,由于加工参数不同,近表面的变形层结构有很大差异。

(2) 不同表面加工处理后材料的抗腐蚀能力存在显著差异,这是由近表面变形结构和残余应力差别大造成的。在工程上表现为,相同表面光洁度、不同加工工艺参数下,材料的抗腐蚀能力存在明显差异。换句话说,表面光洁度不能完整表征材料抵抗腐蚀与应力腐蚀的能力。影响腐蚀速率和应力腐蚀裂纹萌生,很大程度上取决于表面变形层的性质。不锈钢和镍基合金表面纳米化增加了晶界数量,会在腐蚀初期加速氧化膜的生成;当腐蚀深度超过纳米晶层,或者择优腐蚀超过纳米晶层厚度,在表层纳米晶层下面的变形层,包含变形带、机械孪晶等变形结构,对应力腐蚀裂纹萌生起决定作用,因此降低构件应力腐蚀风险的有效途径是通过调整机加工参数,降低近表面剧烈变形发生。

(3) 对于某些承压和表面光洁度要求高的部件,电解抛光是较好的表面处理方法。电解抛光和SiO2机械抛光不锈钢样品的长期腐蚀速率接近;对镍基合金而言,电解抛光表面会形成富Cr贫Ni、Fe层,富Cr层保护膜会阻止O向内扩散,降低电解抛光表面的腐蚀速率。

(4) 划伤表面形成高能区并优先发生氧化和溶解;划伤过程中产生的滑移台阶、微裂纹以及变形晶界都成为应力腐蚀裂纹优先萌生的位置;划伤局部应力腐蚀裂纹数量与划伤深度正相关。对于某些制备、装配环节,例如在蒸汽发生器插管、燃料包壳组装过程中,在蒸汽发生器传热管和包壳管表面产生的不可避免的划伤,应当尽量控制划伤深度,避免过早发生应力腐蚀裂纹萌生。

(5) 在辐照、腐蚀、应力的联合作用下表面形成滑移台阶,该位置优先产生腐蚀或萌生裂纹。辐照促进表面滑移台阶和晶界处局部变形,且晶界和滑移台阶处残余应变集中程度随辐照剂量增加而增加,局部应变明显加速腐蚀。随着辐照剂量增加,辐照促进应力腐蚀敏感性升高。

材料表面状态明显影响核电设备的腐蚀、应力腐蚀开裂以及辐照促进应力腐蚀开裂的速率,这对于长寿命、高安全性要求的核电设备而言非常重要。尽管现有研究结果的基本结论对核电行业已经有一定帮助,也通过理论计算从科学层面得到更深入的认识,为了使得核电设备更加安全、并以更低成本运行,还有很多研究工作值得深入开展,对未来工作的建议包括:(1) 核电用装备涉及的材料多,不同材料因特性不同而存在表面状态影响的明显差异,故而需要进一步以材料基因组方法,补充其他核用结构材料与功能材料的研究结果,例如燃料包壳材料的表面光洁度控制如何做到经济性与安全性的统一;(2) 注重多因素复杂环境中的实验研究,特别是材料、化学、力学、辐照的交互作用认识有待进一步加深,既需要更多的实验证据,又需要理论计算;(3) 核电装备新制造工艺(例如增材制造、构筑成形等)对表面状态的敏感性尚待开展;(4) 核用新材料(例如高熵合金、事故容错燃料包壳材料等)的表面状态如何影响腐蚀、应力腐蚀与辐照促进应力腐蚀。通过上述研究,逐步提出优化的核电关键材料与装备的制造工艺,进一步形成核电材料与装备的制造控制标准,为保障核电站装备的长寿命、高安全性与经济性奠定技术基础。

致谢

感谢彭群家研究员、张志明研究员、明洪亮研究员等同事的讨论与积极贡献;感谢孟凡江博士、韩姚磊博士、闫红林博士、邓平博士、郭跃岭博士、吴斌等研究生在实验研究中的努力贡献。

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将电解抛光态690TT合金样品在325 ℃, 15.6 MPa,含1500 mg/L B, 2.3 mg/L Li, 2.5 mg/L H<sub>2</sub>的高温高压水中连续浸泡720 h后, 取出一半样品用于腐蚀产物的分析, 其余样品继续在含2.0 mg/L O<sub>2</sub>的该高温高压水中连续浸泡720 h. 采用SEM, GIXRD和TEM分析了在上述2种条件下样品表面生长的氧化膜的微观结构. 结果表明, 电解抛光态690TT合金在单一溶氢的高温高压水中表面生长的氧化膜具有双层结构: 外层是分散的富含Ni和Fe大颗粒氧化物和富含Ni的疏松的针状氧化物; 内层是近连续的富含Cr的氧化物; 内外层氧化物均具有尖晶石结构. 在溶氢/溶氧的溶液中连续浸泡后, 样品表面生长的氧化膜也具有双层结构: 外层的形貌、化学组成和物相结构与在单一溶氢条件下生长的氧化膜相似, 仅针状氧化物的长度明显增加; 而氧化膜内层变成了纳米尺寸的NiO. 后期溶解氧扩大了电位-pH图中含Ni的氧化物稳定存在的相区, 促进了外层富含Ni的针状氧化物的快速生长; 更加重要的是, 溶解氧提高了含Fe和Cr氧化物的腐蚀电位, 促进了在溶氢条件下生长的内层富Cr氧化物的溶解, 破坏了氧化膜的保护性结构, 提高了电解抛光态690TT合金的腐蚀速度. 在一回路溶氢/溶氧连续浸泡过程中, 电解抛光处理并不能降低690TT合金的腐蚀速度.

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The microscopic residual stresses beneath scratches on thermally treated (TT) UNS N06690 have been measured using synchrotron radiation x-ray diffraction; the effect of these residual stresses on initiating stress corrosion cracking (SCC) has been studied in 10% sodium hydroxide (NaOH) + 10 g/L lead oxide (PbO) solution at 330°C. Results show that scratching causes local residual tensile stresses parallel to the scratching direction at the scratched surface and local residual compressive stress normal to the scratching direction beneath the scratch. The residual tensile stresses at the scratched surface will act as a precursor of SCC. The residual compressive stresses beneath the scratch cannot stop crack growth of N06690 TT in 10% NaOH + 10 g/L PbO solution at 330°C.

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Effects of cutting parameter on microstructure and corrosion behavior of 304 stainless steel in simulated primary water

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DOI      [本文引用: 9]

The influence of surface conditions on the corrosion behavior of engineering structures has been paid more attention. However, there is still a lack of systematic research on the effect of cutting parameters on material's microstructure and performance in service. In this paper, the effect of cutting parameters on microstructure and corrosion behaviors of 304 stainless steel in simulated primary water is well investigated. The results show that different cutting parameters can cause the superficial layer a gradient microstructure with nanocrystalized layer on top and deformation band structures underneath. With the similar surface roughness, the deformation microstructure can be very different due to the different cutting parameters. The effect degree on the depth of deformation zone is feed rate > cutting depth > cutting speed. The larger feed rate, lower cutting depth, lower cutting rate may induce a deeper deformation zone. With the increasing depth away from the machined surface, the localized corrosion rate is decreased, and at the same depth the localized corrosion rate along the deformation bands is higher than that along the grain boundaries (GBs). The nanocrystalized surface has a smallest general corrosion rate due to the quick formation of Cr rich oxide film. However, once the corrosion penetrates through this nanocrystalized layer, subsequent preferential corrosion at deformation bands and GBs will dominate and may lead to the significant increase of corrosion rate of the component in high temperature pressurized water.

Zhang Z M, Wang J Q, Han E-H, et al.

Effects of surface machining by a lathe on microstructure of near surface layer and corrosion behavior of SA182 grade 304 stainless steel in simulated primary water

[J]. Corros. Sci. Technol., 2019, 18: 1

[本文引用: 4]

Han Y L, Mei J N, Peng Q J, et al.

Effect of electropolishing on corrosion of nuclear grade 316L stainless steel in deaerated high temperature water

[J]. Corros. Sci., 2016, 112: 625

DOI      URL     [本文引用: 4]

Han Y L, Mei J N, Peng Q J, et al.

Effect of electropolishing on corrosion of alloy 600 in high temperature water

[J]. Corros. Sci., 2015, 98: 72

DOI      URL    

Han Y L, Han E H, Peng Q J, et al.

Effects of electropolishing on corrosion and stress corrosion cracking of alloy 182 in high temperature water

[J]. Corros. Sci., 2017, 121: 1

DOI      URL    

Guo Y L, Han E-H, Wang J Q.

Effects of surface state on the electrochemical corrosion behavior of nuclear grade 316LN stainless steel

[J]. Chin. J. Eng., 2016, 38: 87

郭跃岭, 韩恩厚, 王俭秋.

表面状态对核级316LN不锈钢电化学腐蚀行为的影响

[J]. 工程科学学报, 2016, 38: 87

Guo Y L, Han E-H, Wang J Q.

Effects of surface states on the oxidation behavior of 316LN stainless steel in high temperature pressurized water

[J]. Mater. Corros., 2015, 66: 670

Ming H L, Zhang Z M, Wang J Z, et al.

Effect of surface state on the oxidation behavior of welded 308L in simulated nominal primary water of PWR

[J]. Appl. Surf. Sci., 2015, 337: 81

DOI      URL    

Ming H L, Zhang Z M, Wang S Y, et al.

Short time oxidation behavior of 308L weld metal and 316L stainless steel with different surface state in simulated primary water with 0.1 mg/L dissolved oxygen

[J]. Mater. Corros., 2015, 66: 869

[本文引用: 1]

Guo S, Wang H T, Han E-H.

Computational evaluation of the influence of various uniaxial load levels on pit growth of stainless steel under mechanoelectrochemical interactions

[J]. J. Electrochem. Soc., 2018, 165: C515

DOI      URL     [本文引用: 1]

Wang H T, Han E-H.

Ab initio molecular dynamics simulation on interfacial reaction behavior of Fe-Cr-Ni stainless steel in high temperature water

[J]. Comput. Mater. Sci., 2018, 149: 143

DOI      URL    

Wang H T, Sun X F, Han E-H.

The interactions between high temperature water and Fe3O4 (111) by first-principles molecular dynamics simulation

[J]. Int. J. Electrochem. Sci., 2018, 13: 2430

Sun X F, Wang H T, Han E-H.

Effect of Cr doping on the surface characteristics of Ni metal studied with first-principles calculation

[J]. Acta Metall. Sin. (Engl. Lett.), 2019, 32: 461

DOI     

Yin X R, Wang H T, Han E-H.

Effects of solvation and applied potential on the adsorption behaviors of H, O, OH and H2O on Fe(110) surface

[J]. Surf. Sci., 2020, 691: 121504

DOI      URL    

Yin X R, Sun X F, Wang H T, et al.

Adsorption and dissociation of water on halogen pre-adsorbed Ni(111) and Ni-Cr(111) surfaces: A DFT study

[J]. Solid State Commun., 2020, 321: 114040

DOI      URL    

Yin X R, Wang H T, Sun S, et al.

Comparative study on the adsorption behaviors of O and Cl on Fe(110) surfaces with different Cr content

[J]. Mater. Today Commun., 2020, 24: 101122

Wang H T, Ding J W, Zhang R F, et al.

Atomistic insights into interfacial reactions of FeCr2O4 oxide films in high-temperature water

[J]. Int. J. Electrochem. Sci., 2020, 15: 8662

[本文引用: 1]

Meng F J, Wang J Q, Han E-H, et al.

Microstructure near scratch on alloy 690TT and stress corrosion induced by scratching

[J]. Acta Metall. Sin., 2011, 47: 839

[本文引用: 4]

孟凡江, 王俭秋, 韩恩厚 .

690TT合金划痕显微组织及划伤诱发的应力腐蚀

[J]. 金属学报, 2011, 47: 839

[本文引用: 4]

Meng F J, Wang J Q, Han E-H, et al.

Stress corrosion crack initiation for scratched alloy 690TT in oxygenated high temperature water

[J]. J. Chin. Soc. Corros. Prot., 2013, 33: 413

孟凡江, 王俭秋, 韩恩厚 .

划伤690TT合金在高温含氧水中应力腐蚀裂纹萌生的研究

[J]. 中国腐蚀与防护学报, 2013, 33: 413

利用划伤技术研究了690TT合金在325 ℃高温含氧硼锂水中的裂纹萌生和生长情况。试样表面和截面显微分析的结果表明,划伤沟槽底部局部萌生了典型的沿晶应力腐蚀裂纹。由于应力集中,在慢速率拉伸阶段划伤沟槽底部产生了机械裂纹,而机械裂纹成为恒载过程中690TT合金沿晶应力腐蚀裂纹萌生和生长的先导。尖端非常接近晶界或者沿着晶界的机械裂纹可继续形成沿晶应力腐蚀裂纹。690TT合金在恒载荷条件下对应力腐蚀开裂仍有一定的敏感性。

Meng F J, Wu B, Lv Y H, et al.

Effect of surface scratch on corrosion behavior of alloy 690TT heat exchanger tubes

[J]. Chin. J. Mater. Res., 2021, 35: 827

DOI     

Three kinds of samples with different scratch depths on the surface of alloy 690TT for heat exchanger tubes are prepared. The microstructure changes caused by scratch and the effect of scratches on the corrosion and SCC behavior were systematically investigated. The results show that severe plastic deformation occurred near the scratch bank and the scratched groove. A large number of sliding steps and tear deformation generated near the scratched bank. The scratch depth had no obvious influence on the morphology, composition and distribution of corrosion products in different areas of scratches. As the scratch depth increased both the number and the length of SCC cracks increased, indicating that the SCC sensitivity of the material increased. Defects such as slip steps and micro cracks produced during the scratching process were likely to be the preferential positions of SCC initiation.

孟凡江, 吴 斌, 吕云鹤 .

表面划伤对690TT合金传热管腐蚀行为的影响

[J]. 材料研究学报, 2021, 35: 827

DOI     

制备三种表面有不同深度划伤的690TT合金传热管试样并观察划伤导致的微观组织变化,研究了表面划伤对腐蚀、应力腐蚀行为的影响。结果表明:在传热管表面划伤的划伤堤和划伤谷附近出现了严重的塑性变形,并在划伤堤附近产生了大量的滑移台阶和撕裂变形征;划伤深度对不同划伤区域腐蚀产物的形貌、成分和分布等没有明显的影响;随着划伤深度的增大SCC裂纹的数量和长度都呈增加的趋势,说明材料的SCC敏感性增强;划伤产生的滑移台阶、微裂纹等缺陷,易成为SCC裂纹优先萌生位置。

Wu B, Ming H L, Zhang Z M, et al.

Effect of surface scratch depth on microstructure change and stress corrosion cracking behavior of alloy 690TT steam generator tube

[J]. Corros. Sci., 2021, 192: 109792

DOI      URL    

Wu B, Meng F J, Zhang Z M, et al.

Stress corrosion behavior of scratched alloy 690TT steam generator tube in chlorine‐containing high‐temperature pressurized water

[J]. Mater. Corros., 2022, 73: 1563

Wu B, Ming H L, Meng F J, et al.

Effects of surface grinding for scratched alloy 690TT tube in PWR nuclear power plant: Microstructure and stress corrosion cracking

[J]. J. Mater. Sci. Technol., 2022, 113: 229

DOI      [本文引用: 1]

Alloy 690TT tube samples with different scratch depths were repaired by grinding treatments using abrasive papers of two different particle sizes. The microstructure and stress corrosion cracking (SCC) behavior were studied in detail. During grinding, the plastic accumulation zone vulnerable to SCC was removed. Meanwhile, some residual slip steps remained in the scratched area. Corrosion tests lasting 1000, 2000, 3000, and 4000 h show that the sensitivity and risk of SCC in the scratched area are decreased by grinding. Treatment using abrasive particles of a smaller size is more effective. Nevertheless, deep scratches remained hazardous even after the grinding.

Deng P, Peng Q J, Han E-H, et al.

Study of irradiation damage in domestically fabricated nuclear grade stainless steel

[J]. Acta Metall. Sin., 2017, 53: 1588

DOI      [本文引用: 1]

<p>The radiation-induced segregation (RIS) and microstructure evolution such as dislocation loops and cavities are major microstructural causes for the irradiation-assisted stress corrosion cracking (IASCC) of austenitic stainless steel (SS) core components. While a couple of studies have been reported on the irradiation induced damage in nuclear grade (NG) austenitic SS, the evolution of dislocation loop density and size and its correlation with the mechanical properties have still remained incompletely understood. In addition, the correlation between the segregation at the grain boundary and that at the dislocation loop has received limited attentions. In particular, there is still a lack of a systematic study of the irradiation damage in domestically fabricated NG austenitic SS. In this work, the proton-irradiation induced microstructural damage in domestically fabricated 304NG SS was characterized, in an effort to correlate the RIS and the dislocation loop density and size with the irradiation dose, as well as the dislocation loop density and size with the radiation-induced hardening. The results revealed that the radiation-induced microstructure damage was mainly dislocation loops with a few micro-voids. The loop density was in the order of 10<sup>22</sup> m<sup>-3</sup> with an average size of <10 nm. The square root of the product of loop density and size (<i>Nd</i>)<sup>0.5</sup>, scaled linearly with the square root of irradiation dose with a factor of 6.8×10<sup>3</sup> dpa<sup>-0.5</sup>mm<sup>-1</sup>. The loops were believed to be mainly responsible for the hardening in 304NG SS, which also scaled linearly with (<i>Nd</i>)<sup>0.5</sup> with a factor of 1.16×10<sup>-2</sup> HV<sub>0.025</sub>mm. A comparative analysis about the segregation at the grain boundary and at the dislocation loop was conducted. While the depletion of Cr and enrichment of Ni at the dislocation loop and grain boundary showed no difference, the enrichment of Si at the dislocation loop could be of about 6 times of that at the grain boundary. In addition, the loop density and loop size, as well as RIS and radiation-induced hardening were all increased by a higher dose and tended to saturate by a dose of 3.0~5.0 dpa.</p>

邓 平, 彭群家, 韩恩厚 .

国产核用不锈钢辐照损伤研究

[J]. 金属学报, 2017, 53: 1588

[本文引用: 1]

Deng P, Peng Q J, Han E-H, et al.

Effect of irradiation on corrosion of 304 nuclear grade stainless steel in simulated PWR primary water

[J]. Corros. Sci., 2017, 127: 91

DOI      URL     [本文引用: 1]

Deng P, Peng Q J, Han E-H, et al.

Effect of the amount of cold work on corrosion of type 304 nuclear grade stainless steel in high-temperature water

[J]. Corrosion, 2017, 73: 1237

DOI      URL    

Deng P, Sun C, Peng Q J, et al.

Study on irradiation assisted stress corrosion cracking of nuclear grade 304 stainless steel

[J]. Acta Metall. Sin., 2019, 55: 349

DOI     

Irradiation assisted stress corrosion cracking (IASCC) of austenitic stainless steel core components is one major concern for maintenance of nuclear power plants. Previous studies on the IASCC had mainly focused on the effect of irradiation on changes in deformation modes and interaction of dislocation channels with grain boundary. The role of corrosion in IASCC, however, has not received sufficient attentions. In the process of stress corrosion cracking (SCC), corrosion occurs simultaneously with localized deformation in the vicinity of the crack tip. This indicates that corrosion is one of the potential contributors to IASCC. In this work, IASCC of proton-irradiated nuclear grade 304 stainless steel (304SS) was investigated. The IASCC tests were conducted by interrupted slow strain rate tensile (SSRT) tests at 320 ℃ in simulated primary water of pressurized water reactor containing 1200 mg/L B as H3BO3 and 2.3 mg/L Li as LiOH·H2O, with a dissolved hydrogen concentration of 2.6 mg/L. Following the SSRT tests, the localized deformation, corrosion and IASCC of the specimens were characterized. The results revealed that increasing the irradiation dose promoted residual strain accumulation at slip steps and grain boundaries of nuclear grade 304SS. Since the slip step usually transmitted or terminated at the grain boundary, it eventually promoted localized deformation at the grain boundary. Specially, the slip step transmitted at grain boundary led to slip continuity at the grain boundary. In contrast, a slip discontinuity was observed at the grain boundary where the slip step terminated, which caused a much higher strain accumulation by feeding dislocations to the grain boundary region. Further, formation of the slip discontinuity was related to the Schmidt factor pair type of the adjacent grains. The irradiation resulted in a depletion of Cr and an enrichment of Ni at grain boundary, while the magnitude of Cr depletion and Ni enrichment increased with increasing the irradiation dose. Following the SSRT tests, intergranular cracking was observed on surfaces of the irradiated specimens, while the number of the cracks was increased by a higher irradiation dose and applied strain. This suggested a higher IASCC susceptibility of nuclear grade 304SS in the primary water. Meanwhile, significant intergranular oxidation ahead of the crack tip was observed, while both the width and length of the oxide were larger at a higher irradiation dose. The synergic effect of irradiation-promoted deformation and intergranular corrosion was the primary cause for the IASCC of the irradiated steel.

邓 平, 孙 晨, 彭群家 .

核用304不锈钢辐照促进应力腐蚀开裂研究

[J]. 金属学报, 2019, 55: 349

Deng P, Han E-H, Peng Q J, et al.

Corrosion behavior and mechanism of irradiated 304 nuclear grade stainless steel in high-temperature water

[J]. Acta Metall. Sin. (Engl. Lett.), 2021, 34: 174

DOI      [本文引用: 1]

Deng P, Peng Q J, Han E-H, et al.

Proton irradiation assisted localized corrosion and stress corrosion cracking in 304 nuclear grade stainless steel in simulated primary PWR water

[J]. J. Mater. Sci. Technol., 2021, 65: 61

DOI      [本文引用: 5]

Localized deformation and corrosion in irradiated 304 nuclear grade stainless steel in simulated primary water were investigated. The investigation was conducted by comparing the deformation structure, the oxide scale formed at the deformation structure, and their correlation with cracking. The results revealed that increasing the irradiation dose promoted localized corrosion at the slip step and grain boundary, which was primarily attributed to the strain concentration induced by enhanced localized deformation and depletion of Cr at grain boundary. Further, a synergic effect of the enhanced localized deformation and localized corrosion at the slip step and grain boundary caused a higher cracking susceptibility of the irradiated steel.

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