Journal Pre-proof A review of fretting study on nuclear power equipment Zhen-bing Cai, Zheng-yang Li, Mei-gui Yin, Min-hao Zhu, Zhong-rong Zhou PII:
S0301-679X(19)30609-7
DOI:
https://doi.org/10.1016/j.triboint.2019.106095
Reference:
JTRI 106095
To appear in:
Tribology International
Received Date: 9 August 2019 Revised Date:
13 November 2019
Accepted Date: 29 November 2019
Please cite this article as: Cai Z-b, Li Z-y, Yin M-g, Zhu M-h, Zhou Z-r, A review of fretting study on nuclear power equipment, Tribology International (2020), doi: https://doi.org/10.1016/ j.triboint.2019.106095. This is a PDF file of an article that has undergone enhancements after acceptance, such as the addition of a cover page and metadata, and formatting for readability, but it is not yet the definitive version of record. This version will undergo additional copyediting, typesetting and review before it is published in its final form, but we are providing this version to give early visibility of the article. Please note that, during the production process, errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain. © 2019 Published by Elsevier Ltd.
Graphical Abstract
Typical positions of fretting wear in steam generator.
A review of fretting study on nuclear power equipment Zhen-bing Cai, Zheng-yang Li, Mei-gui Yin ,Min-hao Zhu, Zhong-rong Zhou Tribology Research Institute, Southwest Jiaotong University,610031,Chengdu, China Abstract: Nuclear power plants, working in extremely harsh environment, primarily in the form of high-speed fluid flow, circulate through complex systems. Serious tribological problems can occur when a small amount of nuclear energy is converted into mechanical energy in the components (e.g., fuel-rod cladding, tube of the heat exchange systems). With the increase of the service life of nuclear power equipment, a considerable number of nuclear power equipment or structure failures occur one after another. Although the influencing factors are different, fretting damage is one of the important factors. Fretting damage has strong concealment and high risk, and it is often the main cause of component failure. Thus, improving the reliability of nuclear power equipment, extending their life, and optimizing their structure are important. In recent decades, many scholars have studied fretting wear, fretting fatigue, and fretting corrosion behavior in nuclear power equipment. Accordingly, they have solved many problems, accumulated a lot of experience, and put forward many criteria. In this article, the research status of fretting damage in key equipment and structures of nuclear power plant is reviewed. Keyword: nuclear powder, fretting, SG tube, fuel rod cladding 1. Introduction Electric power generation usage is a key factor of advances in the industry, agriculture, and socioeconomic level of living [1]. Electrical energy can be generated from burning mined and refined energy sources, such as coal (37.9%), natural gas (26.6%), oil (3.0%), and nuclear (10.1%), and from harnessing energy sources, such as hydro(15.8%), biomass (2.2%), wind (5.5%), solar (2.4%), and geothermal and wave power (0.4%). According to the report of the World Nuclear Association in July 2019, the global nuclear power generation is steadily growing. In 2018, the nuclear power generation reached 2563 TWh, an increase of 1.7% compared with 2519 TWh in 2017, and the per capita nuclear power consumption was 10.3%. China has made rapid progress in nuclear power generation, ranking third in the world. However, in 2018, nuclear power generation accounted for only 4.2% of total power generation, higher than 2017, but far below the global average of 10.3%. On the development 1/32
speed of nuclear power generation, China has the fastest development, with 13 nuclear reactors under construction, 43 was proposed. Table 1 Nuclear power plant reactors in some countries (June 2019) [2] Total Nuclear Power in 2018
June,2019 (Reactors) In operation
Under
Proposed
construction TWh
%e
Num
MWe
Num
MWe
Num
MWe
USA
808.0
19.3
97
98699
4
5000
3
2550
France
395.9
71.7
58
63130
1
1750
0
0
China
277.1
4.2
46
44688
12
11091
43
50900
Russia
191.3
17.9
36
29139
6
4973
24
25810
Korea
127.1
23.7
24
23231
4
5600
0
0
Germany
71.9
11.7
7
9444
0
0
0
0
U.K
59.1
17.7
15
8883
1
1720
3
5060
World
2563
10.3
447
399224
55
58894
111
121829
The world’s first nuclear power plant was put into operation 70 years ago. Fig 1 shows the development of nuclear power plants. At present, nuclear reactors in commercial operations mainly belong to the second- and third-generation nuclear reactors. To enable secured, efficient, and environmentally friendly nuclear energy than the existing reactors, the fourth-generation nuclear reactors have been actively developed by various research institutes to be applied in commercial operations before 2030 [3, 4].
Fig. 1. Development of nuclear power plants In nuclear power equipment, several kinds of components or materials are subjected to wear phenomena [5]. Fuel, steam generators, pipelines, and other systems involve many connectors. Wear of materials and interface loosening or the gap caused by vibration, heating, and heat transfer are inevitable. Taking pressurized water reactor (PWR) system as an example, the service life of a steam generator, which relies on a tube heat exchanger, is the most significant issue in nuclear power plants. A great number of steam generators are removed from the equipment to be repaired or 2/32
replaced due to flow-induced vibration (FIV), which initiates fretting that occurs during a heat exchange. Fretting with small-amplitude oscillatory motion occurring between tubes and their supports (or antivibration bars) [6]. Another component that undergoes fretting is the fuel cladding. The service environment of fuel cladding is more complex, involving high temperature and high-pressure water, intense neutron irradiation, electrochemistry, complex mechanical stress, and fission gas of nuclear fuel. The FIV cause small relative motions between the fuel rod and spacer grids. Grid-to-rod fretting (GTRF) is the leading cause of the fuel failure of PWRs and is one of the problems addressed by the Consortium for Advanced Simulation of Light Water Reactors to guide its efforts and develop a virtual reactor environment [7]. GTRF may produce wear of the rod cladding that can lead to the exposure of fuel pellets if not caught early enough (such situations are called “leakers”). Leakers are a significant concern for PWR designers and plant operators [8, 9]. More than 70% of leakers result from GTRF wear in PWRs. In this paper, the research status of nuclear power materials, mainly heat transfer and fuel systems, has been reviewed in the recent 20 years. The test materials, test methods, and research hotspots are also analyzed and summarized. 2 Fretting test method and test device The actual nuclear power equipment service environment is complex and harsh. Hence, the simulation research and analysis in the laboratory cannot easily achieve actual working conditions. In addition, obtaining the parameters of evaporator or fuel chamber components, such as vibration displacement, vibration frequency, and actual contact conditions between the support interfaces, is difficult. Except failure analysis, most research on the fretting of nuclear power materials is based on material-level experimental or numerical analysis. The research on fretting can be divided into fretting wear, fretting fatigue, and fretting corrosion. At present, many studies in the field of fretting wear are available. In the literature, fretting wear models have historically taken several forms: Mechanical eccentric cylinder or cam [10, 11], Hydraulic pressure [12, 13], Piezomotors [14, 15], Electromagnetic fields [16–18], Voice coil motor [19–20], Improvement by fatigue tester [21]. Mechanical eccentric cylinders have lower displacement output accuracy and wider displacement range, hydraulic pressure testers have smaller displacements and lower frequencies, and piezomotors and voice coil motor can provide small 3/32
displacement and high frequencies. The tester improved from the fatigue machine’s accuracy of displacement control is poor, and the fixture installation is not convenient enough. Generally, the installation and operational performance of the clamp in the horizontal mode is better than those in the vertical mode in the material testing processing. Thus, the use of the horizontal mode in fitting liquid containers, arranging motors and sensors, and clamping samples during tests is convenient.
(a) Eccentric model[10]
(b) Hydraulic pressure[12]
(c) Piezomotor[14]
(d) Electromagnetic[16]
(e) Voice coil motor[18-19] (f) Improvement by fatigue tester[21] Fig. 2 Fretting wear test machine with various driving modes Compared with fretting wear, fretting fatigue and fretting corrosion are less studied. Fretting fatigue. Fig 3a [22, 23] shows a typical schematic diagram and photograph of fretting fatigue testing apparatus in the room temperature test. Base plates were fastened on the main frame of the system. Loading screws were placed through the proving ring contact on the back of the arm whose root was welded to the 4/32
base plate. The inner tip of the arm fits in to the conical groove on the back of the bridge pad. As the loading screw was tightened, the tip of the arm pushed the pad in the ward and the contact force on the fatigue specimen increased. Many fretting corrosion tests only add a solution immersion chamber and an electrochemical measurement system on the fretting wear test equipment (Fig. 3b). Research institutes have recently developed micro-motion research equipment with an enclosed high-temperature fluid environment, which is near the service environment. However, the sensor cannot be implanted into the test system because of high temperature and pressure, which makes the tribological parameters of the actual interface difficult to obtain [24–26]. Researchers have to rely on the physical and chemical properties of the tested material after the end of the experiment.
(a) Fretting fatigue tester [22] (b) Fretting corrosion [23] Fig. 3 Fretting wear and fretting fatigue test machine 3 Fretting research in steam generator tubes 3.1 SG tube materials In currently operating nuclear power plants, steam generators, which always include a tubular evaporator, are primary responsible for the heat exchange between the primary and secondary circuits [27]. The service environment for steam generator tubes is exceptionally harsh, mainly due to high temperature, strong stresses, chemical corrosion, and neutron irradiation [28–29]. The heat transfer area of the steam generator in most commercial nuclear power plants are always composed of a large number of small-diameter thin-walled seamless U-shaped tubes. The outer diameter of these heat transfer tubes are usually approximately 22, 19, and 15.8 mm, and the corresponding wall thickness are approximately 1.27, 1.09, and 0.86 mm (Fig. 4).
Fig. 4. Dimensions of varied steam generator tubes Excellent structural characteristics and mechanical properties of steam generator 5/32
tubes play a key role in the heat transfer safety, capacity, and efficiency of nuclear power plants. Since the nuclear power plants have been put into operation, a considerable amount of effort has been made to improve the mechanical properties and corrosion resistance of steam generator tubes. In the 1960s, the heat transfer tubes of many Western press water reactors were manufactured by 304 and 316 austenitic stainless steels. After a period of service, they found that these materials are very sensitive to intergranular and stress corrosion under liquid mediums that contain chloride. To remedy this situation, most of them were substituted by the Inconel-600 (I-600MA) alloy that is only treated by factory annealing. In the mid-1970s, researchers found that erosion, pitting, intergranular corrosion, and other failure phenomena sequentially happen on this kind of tubes. To resolve this problem, refined craftwork has been applied to improve the intrinsic resistance of Inconel-600 alloy, and then Inconel-600TT was used since the mid-1980s. After the 1990s, the Inconel-690 alloy and Incoloy-800 were derived and used to manufacture heat exchanger tube production. All these materials were treated by some special heat treatment processes [30–33]. Figure 5 exhibits the evolution of steam generator tubes with time.
Fig. 5. Evolution of steam generator tube materials and hot working parameters. Fourth-generation nuclear reactor includes three different thermal neutron reactors (supercritical water reactor, very-high-temperature reactor, and molten salt reactor) and three fast neutron reactors (gas-cooled, sodium-cooled, lead-cooled fast reactors). The definitions of these new nuclear reactors differ from one another in terms of their neutron spectrum, coolant, and moderator [34]. Table 2 shows the materials that have been widely studied and are likely to be applied in the practical 6/32
employment of fourth-generation nuclear reactors [35–37]. Table 2. Fourth-generation nuclear reactors and their materials in heat exchange
3.2 Fretting behaviors of steam generator tubes In practical service, the working environment for steam generator tubes is complex and harsh. The difference in pressure inside and outside the tubes, neutron irradiation, and various fretting wears and fatigue behaviors can easily be identified among heat exchange tubes because of FIV. Furthermore, high temperature and water pressure containing boric acid and lithium hydroxide have corrosive actions to steam generator tubes. Thus, the fretting corrosion is common among steam generator tubes, and such damages are difficult to overcome and avoid. Figure 6a shows some typical wear positions that often occur between heat transfer tubes and their support structures. To alleviate and avoid the fretting wear and corrosion of steam generator tubes, researchers have paid much attention to the thorough and detailed studies of these phenomena and problems under different conditions [38].
7/32
(a)Typical positions of fretting wear in steam generator
Fig. (b)Fretting researchon the heat tube materials Fig.6 Fretting in steam generator and heat tube materials Considerable research works on the fretting behaviors and performance of steam generator tube materials, fretting wear, fretting fatigue, and fretting corrosion are available in the literature. To make the experimental studies similar to actual service conditions of heat exchange tubes, different experimental variables have been simulated and implemented for investigation. Figure 6 b exhibits the experimental variables that researchers have widely studied under their real research works. A lot of research works on the fretting behaviors of various steam generator tubes have been performed, and some remarkable results have been achieved. These research works can be roughly divided into five parts based on the test environment: 8/32
(a) Dry condition room temperature in air: The influence of displacement amplitude, sliding frequency, normal force, and wear cycles have been widely studied by researchers. Almost all results indicate that the friction force, wear volume, and fretting mode change with the amplitude [39–41]. Yun et al. concluded that the wear mode does not change with increasing sliding frequency [42]. Li et al. found that the wear degree and mechanism of alloy tubes slowly change with the increase of wear cycles, and all these will rapidly change after a particular number of cycles [43]. Xin’s results revealed that the normal force can affect the material transfer, which occurs with different slip regimes [44–45]. Soria et al. found that the dominant wear mechanism mainly depends on the particular composition of the mated wear materials [46]. (b) Dry condition with different air temperatures: Heat exchange tubes are serviced in high-temperature environments. Xin et al. studied the influence of displacement amplitude and wear cycles on the structure of wear scars [47, 48]. They found that the content of oxygen can influence the characteristics of nanostructured tribo-layers and therefore affect the wear degree and mechanism of materials [49]. Mi’s results found that the wear volume in 90 °C is more serious than that of 200 °C and 285 °C [13]. Zhang et al concluded that fretting running regimes are basically unaffected by temperature [50, 51]. Kwon et al. studied the fretting wear behaviors of Inconel-600 under room and 320 °C temperatures. The wear groove that formed in high temperature was much rougher than that formed in the room temperature, and the fatigue strength was not significantly different [22]. (c) Water condition room temperature: Xin et al. compared the wear behaviors of Inconel-600 alloy tubes under the conditions of dry air and deionized water. They found that the white etching layer is more difficult to form in deionized water than that in dry condition [52]. Li et al. studied how the polarization condition influence the wear behaviors of alloy tubes and found that the crack nucleation and propagation, microstructure evolution and damaged mechanisms, COF, and wear volume strongly depend on the polarization condition [53]. (d) Different water temperatures/air condition: In practical conditions, the steam generator tubes are always serviced in high-temperature and water pressure solutions. Ming and Xin investigated the effect of normal force on the fretting wear behaviors of alloy tubes under 288 °C pressed water. They all found that normal force significantly influences the degree of wear and failure mode [15, 54]. Guo found that test samples mainly exhibit abrasive wear when the sliding amplitude or normal load is low; however, delamination wear dominates when either of the element is increased [55]. Liao concluded that the fretting fatigue life of Inconel-600 can be in high temperature water [56]. Lai et al. found that the wear volume of test samples increased with the water temperature before 90 °C and then decreased beyond that temperature [24, 25]. Xin et al. found that sliding frequency has little effects on the 9/32
oxide phases of worn surfaces; however, the increasing frequency can enhance the thickness of oxide film, which can accelerate the fretting corrosion of test samples [57]. Guo found that the higher the chromium content of mated wear material, the better the wear resistance of the Inconel-690 alloy tube [24]. Guo separately compared the wear behaviors of alloy tubes under argon and water conditions and found that high temperature water can attribute to the form of oxide layer and transportation of wear particles in the fretting process and finally strengthen the wear resistance of materials [24]. (e) Other solutions: Wang investigated how the PH value of solution affects the wear behavior of alloy tubes and the results showed that the corrosion rate decreased as the PH values increase from 4 to 13. The Inconel-690 alloy became the active metal at a pH value of 13 [58]. Li et al. found that the layer of wear scar will be oxidized by the chloride ion [59]. Table 3 Test materials and parameters. Tubes
Friction
Lubrication
Temperature
Displacement
Frequency
pair
condition
℃
(µm)
(Hz)
Ref
In600
GCr 15
dry
RT
30-150
20
[40.45]
In690
409SUS
dry
RT
25-300
10-60
[44]
405SS
dry
RT,90,200,285
100,200
5
[12]
405SS
8.6 MP water
285
20-100
5
[59]
405SS
2 MPa water
RT, 90 °C
100
5
[26]
10 MPa water
285 °C
100
5
18 MPa water
350 °C
100
5
405SS
8.6MPa water/Agon
285 °C
100
5
[25]
304SS
PH1-4,PH7,PH10,13.
RT
30
20
[66]
304SS
3.5% NaCl solution
RT
100
20
[67]
304SS
Dry and water
RT
Impact
5
[18]
1Cr13
dry
RT,100,300
100,200
10,50
[54]
In690
304SS
dry
RT
15-75
-
[41]
TT
304SS
dry
RT
45
20
[46,47]
304SS
dry
220
90
20
[49]
304SS
dry
RT,320
15-75
20
[50]
304SS
5 vol%-21% oxygen
320
150
20
[51]
304ss
Water, 15 MPa
288
96,139.165
30
[15]
304ss
dry
RT
15-75
20
[55]
Inconel
AISI304
dry
RT
75
15
[48]
800
AISI1060
In600 MA
10/32
304SS
dry
RT,300.400
2-40
2
[53]
(a) Damage evolution with increasing cycles[43] (b) Cross sections of worn scar [47]
(c) Schematic of the typical worn surface [47]
(d) Damage evolution [49] Fig. 7 Results of the fretting wear scar
Research works about the impact or impact–sliding wear behaviors of various steam generator tubes have been carried out. Cai et al. used a self-made test rig to study the impact wear behaviors of alloy tubes under different test conditions or parameters [60–62]. Souilliart et al. investigated the influence of incidence energy and angle on the impact wear behaviors of steam generator tubes under dry and water environments [63–64]. For the impact–sliding wear, Cai et al. designed a test rig to study the effect of impact and sliding velocities on the wear behaviors of Inconel-690 alloy tubes [65]. Cheng et al. studied how the ratio of impact and sliding frequency and displacement amplitude affect the wear behaviors of heat exchange tubes based on an impact–sliding wear test rig [66, 67]. Figure 8 shows the variables that have 11/32
been investigated during the impact or impact–sliding wear test of steam generator tubes.
Fig. 8. Impact and impact–sliding wear[66-68] 3. 3 Surface strengthening processes for anti-fretting Researchers have proposed some technologies for metal surface intensity to further improve the wear performances and some mechanical properties of alloy tubes. Figure 9 summarizes the surface hardening process that has been applied to improve some mechanical properties of steam generator tubes. Hu et al. studied the influence of different reductions of cold rolling on the fretting wear behavior and mechanism of Inconel-690 alloy at 320 °C in air. The grains were horizontally elongated along the rolling direction as the degree of cold rolling increased (Fig. 10 a). They found that the damage mechanism of test samples changed from oxidation, delamination, and abrasive wear to adhesive wear with the increase of cold rolling reduction [68]. Lee et al. studied how the temperature and time of aging treatment affect the wear behaviors of alloy tubes. No carbide was found after aging treated for 1 h, and the carbides that precipitated along the grain boundary became coarse as the treated time increased to 10 h (Fig. 10b). They found that the wear behavior of test samples was significantly affected by the carbides that precipitated during the treatment process. The friction coefficient and wear volume increased with the carbide precipitation [69, 70]. Zhang et al. investigated that the grain size of the Inconel-600 alloy increased and its hardness decreased as the solution temperature increased. During the wear process, the bigger the grain size, the larger the wear volume; however, the bulk hardness played a little role in the wear volume [71]. From the cross section of wear scars, the length of the main crack distinctly increases at a solution temperature higher than 1000 °C (Fig. 10 c). After alloy tubes treated by ultrasonic surface rolling process 12/32
(USRP), a hardening of surface up to a certain depth is observed. Microstructural evolution and hardening are attributed to the increase in density of various dislocation structures [72]. When the same wear condition is suffered, the wear resistance of the USRP treated sample is obviously better than that of the untreated one (Fig. 10d).
Fig. 9. Processes for alloy tube surface strengthening
(a) Cold rolling [68]
(b) Aged treated [69]
13/32
(c) Cross section in high temperature [70] (d) Treated USRP [65] Fig. 10. Wear characters of alloy tubes 3.4 Development trend of the fretting steam generator tubes in the future The materials used for heat transfer tubes of nuclear power evaporators have gone through the evolution process of Inconel 600, Incoloy 800 and Inconel 690. Inconel 690 is widely used in the heat transfer tubes of nuclear power evaporators because of its outstanding oxidation resistance and stress corrosion resistance. As for the fretting research of heat transfer tubes, there may be the following trends in the future: (a) The complex fretting forms of 690 alloy were studied, such as fretting damage mechanism under impact-tangential coupling, fretting corrosion behavior and damage mechanism, fretting damage under abrasive action. (b) Heat transfer tube of the fourth generation reactor, fretting under the action of molten metal medium (such as metal sodium, lead bismuth environment) (c) The application of surface engineering technology in heat transfer tube, including fretting damage behavior, friction and wear resistance behavior.
. Fretting on fuel rod system Fuel rods are the key components of a light-water reactor’s fuel assembly. Fuel rods are composed of cladding tube in which uranium dioxide pellets are stacked [73, 74]. Cladding tube has a length of approximately 4 m, a diameter of approximately 9.5 mm, and wall thickness of approximately 0.5 mm. The fuel rods are supported by spacer grids, and the rods directly contact with the springs and dimples. The most important function of cladding tube is to prevent fission products from escaping and efficiently dissipate heat [75]. 14/32
The high temperature, high pressure, high radiation, and severe operating condition in the reactor cause the failure of cladding tube. According to the survey, fuel rod failure is mainly caused by the GTRF and debris-induced fretting wear in Fig. 11 [76].The GTRF was caused by excessive FIV, and this vibration is restrained by its contact with the springs and dimples of the spacer grid [77–78]. The excessive FIV may be divided into external and internal vibrations. The external vibrations were caused by reactor internals, inter fuel-assembly gaps, and fuel assembly-shroud gaps, whereas the internal vibrations were due to inadequate spacer grid mixing vane designs, spacer grid strap designs, water-to-fuel volume ratios, fuel rod and assembly stiffness, and bottom and top nozzle flow hole designs. GTRF will cause wear damage of the cladding tube in Fig. 12, which may lead to the wearing out of the cladding tube in serious cases. If such case happens, then radioactive fission gases in the fuel rods would be released to the coolant, which increases the radioactivity level of the coolant. Even if a perforation does not occur, thickness reduction of cladding tube caused by wear can decrease the strength of the fuel rods [79–80].
(a) 2002 to 2006 (b) 2007 to 2011 Fig. 11 Percentage of fuel failure in PWRs all over the world [76]
Fig. 12 Fretting damage of cladding tube in PWRs [79-80] 15/32
4.1 Evolution of cladding materials The preparation of cladding materials is important, and the materials must possess excellent corrosion, fretting wear, creep, and high-temperature thermal oxidation resistance property in the aggressive reactor environment. Zirconium alloys are widely used as a fuel cladding material in the world because of low thermal neutron capture cross section of 0.18×10-28 m2, good corrosion resistance, good compatibility of uranium fuel, and good machining performance [81–82]. Figure 13 shows the evolution of cladding materials developed by the United States, Korea, and China. Zirconium alloys have been developed to three types: Zr–Sn, Zr–Nb, and Zr–Sn– Nb. Table 4 shows the typical cladding materials that have been successfully used and tested in the world [83, 84]. In the 1950s, Zr-2 alloy was developed in the United States, which has a good high-temperature water and steam corrosion performance and successfully used as fuel cladding material [85]. However, the presence of Ni increases the hydrogen absorption of Zr-2 alloy [86]. Therefore, Zr-4 alloy was developed by decreasing Ni and increasing Fe content on the basis of Zr-2 alloy. Zr-2, Zr-4, and Zr-1Nb are called as first-generation zirconium alloys. With the development of smelting technology, Sn content in zirconium alloy can be controlled at a lower level. By adjusting the contents of Sn, Fe, and Cr and improving the microstructure of the alloy through heat treatment, an improved Zr-4, namely, low-tin Zr-4 alloy was developed, which is considered a second-generation zirconium alloy [87]. To achieve higher usage requirements, researchers developed Zr–Sn–Nb alloy after combining the advantages of Zr–Sn and Zr–Nb alloys. Zirlo, M5, HANA, and N36 alloys are called as third-generation zirconium alloys [76, 88, 89]. In the 2011 Fukushima nuclear power plant accident, zirconium alloy cladding in the reactor fuel was aggressively oxidized by high-temperature steam generated under accident conditions, resulting in a large amount of hydrogen and heat, which eventually led to a reactor core meltdown and hydrogen explosion [89]. From then on, the development programs of accident-tolerant fuels (ATFs) have been initiated worldwide. ATF program is aimed at the development of alternative cladding and fuel concepts. According to the research and evaluation of different researchers, ATF cladding materials can be classified into ceramic and metallic materials [84, 90, 91]. The metallic materials mainly include FeCrAl and Mo-based alloys. The ceramic materials are mainly represented by SiC/SiC composite materials.
16/32
Fig. 13 Evolution of cladding materials developed by the United States, South Korea, and China Table.4 Chemical element composition of the typical zirconium alloys Country
Alloy
Chemical element composition (w/%) Zr
Nb
Sn
Fe
Cr
Ni
Zr-2
Balance
-
1.2-1.7
0.07-0.20
0.05-0.15
0.03-0.08
Zr-4
Balance
-
1.2-1.7
0.18-0.24
0.07-0.13
0.007
Zr-4 (Low Sn)
Balance
-
1.2-1.5
0.18-0.24
0.07-0.13
-
Zirlo
Balance
1.0
1.0
0.1
-
-
X5A
Balance
0.3
0.5
0.35
0.25
Japan
NDA
Balance
1.0
1.0
0.27
0.16
0.01
France
M5
Balance
1.0
-
-
-
-
Russia
E635
Balance
1.0
1.3
0.4
-
-
Korea
HANA6
Balance
1.1
N18
Balance
0.3
1.0
0.3
0.1
-
N36
Balance
1.0
1.0
0.3
-
-
C7
Balance
1.0
-
0.01 (Fe)
-
-
U.S.A
China
0.05 (Cu)
4.2 Fretting wear of cladding tube in different test conditions The fretting wear mechanism of zirconium alloy has been studied worldwide. In the initial stage, considerable research has been conducted in the dry condition, and this condition can only partially reveal the fretting wear mechanism of the cladding tube. Kim [92–93] studied the fretting wear of Zr-4 alloy with Inconel-600 alloy in the air environment, indicating that wear volume increased with load, slip amplitude, and number of cycles and wear volume was mainly affected by slip amplitude. Attia [94–95] investigated the fretting wear mechanism of Zr-2.5Nb alloy in air at 265 ℃, using a specially designed fretting wear tribometer. A novel approach of the thermal 17/32
and electrical contact resistances was introduced to measure the oxide layer thickness in the fretting interface. Winter [96–97] reported that FeCrAl alloy is an excellent ATF cladding material compared with Zr-4 alloy and SiC/SiC composite material due to its good wear resistance performance. The formation of a protective aluminum oxide and chromium oxide layer can reduce the COF and wear at 350 ℃ under dry fretting conditions. With the development of testing technology, fretting wear test was conducted in an autoclave to simulate the high-pressure water environment in a reactor. Qu [98–100] investigated the effect of water temperature (22 °C, 150 °C, and 204 °C) on the fretting wear behavior of zirconium alloy used in actual PWR and found that the zirconium alloy wear volume rapidly increased with a high water temperature. Zhang [101–102] revealed that the dominant wear mechanisms of SZA-4 alloys in 300 °C pressurized B–Li water condition are delamination and oxidation. Gene [103] investigated the change in surface roughness of wear surface before and after fretting testing in 260 °C water condition and found evidence of plastic deformation and wear debris. Fretting wear test in high-pressure water environment can simulate the actual operating condition and reveal the synergetic action between wear and corrosion. However, sensors (such as force and displacement) are limited and difficult to be applied in to a high-pressure water environment to monitor the state data and fretting run region in real time. 4.3 Effect of spacer grid shape on the fretting wear of cladding tube GTRF behavior is also affected by the design of a spacer grid. Different grids decide the contact mode among the spring, dimple, and fuel rod. Lee and Kim [80, 104–110] designed springs and dimples with different geometric shapes (Fig. 14a) and investigated the effect of supporting structure shape on the fretting wear behavior of zirconium alloys. The results shows that the shape of supporting structures directly decides the contact form (point, line, and surface contacts) and further affect the contact stress, contact area, wear depth, wear area, wear evolution, debris dispersion, fretting region, and wear volume. Kim [111, 112] investigated two spacer grids that have been applied in PWR on the fretting wear behavior of Zr-4 alloy (Fig. 14b). Grid B with conformal contacts shows a better fretting wear resistance than Grid A with point contacts. Hu [113–114] reveals that the wear rate depends on the size of gap between the grid and fuel rod (Fig. 14c) and found that the existence of a critical gap size results in a maximum wear rate. Kovács [115] found that the springs with a larger radius of curvature has a larger contact points and larger contact surfaces (Fig. 14d), which leads to lower wear depth and better fretting resistance behavior. Shin [116– 117] used the homology constraint model and found that maintaining the elastic 18/32
deformation of the spring center can increase the contact area and decrease the fretting wear (Fig. 14e).
(a)
(b)
(c)
(d) (e) Fig. 14 Different shapes of space grid: (a) (b) [80,104–108], (c) [111–112], (d) [113], (e) [114] 19/32
4.4 Impact fretting wear of cladding tube In actual operating conditions, the fuel assembly is subjected to axial and transverse flows of high-speed coolants. Impact, sliding, and impact–sliding movement occur in the cladding tube with spring and dimple (Fig. 15) [110]. Pablo [118] proposed a nonlinear vibration model and calculated the impact force between the rod and supports as approximately 0.2 N. Ko [119] found that the impact fretting on zirconium alloys is correlated with motion parameters, test duration, material combination, and temperature. Kim [108] compared the sliding and sliding–impact motion mode on the wear property of Zr-4 alloy and found that the sliding–impact motion mode shows a larger wear volume. Jones [120] investigated the impact fretting wear behavior on the reactor component in the pressurized CO2 advanced gas-cooled reactor. The impact wear behavior shows a transition from a severe wear to a mild wear at a temperature in the range of 250 °C–450 °C, and the critical temperature depends on the material and test parameters. Fisher [121] found that the wear volume of zirconium alloy under the impact fretting wear condition at temperatures below 150 °C is approximately equal to that above 300 °C but is five to 10 times larger than that in 250 °C–286 °C. Cai [19] studied the effect of diameter– thickness ratio on the impact fretting wear of Zr-4 alloy in a novel low-velocity impact fretting wear test rig. The test rig can provide cycling constant kinetic energy at every impact cycle and measure and record the deformation, loss of kinetic energy, absorbed energy rate, and contact force in real time and each cycle during the impact process. The results showed that under the same tube outer diameter, an increase of tube wall thickness will lead to an increase in contact time and a reduction in peak force, energy absorption ratio, and damage degree. Many researchers just use the tangential fretting wear to evaluate the wear resistance of cladding tube and ignore the impact fretting wear and impact–sliding fretting wear[18-20,61-62,66-67]. However, many studies indicate that impact–sliding fretting wear has a larger wear damage than single impact fretting wear and tangential fretting wear. Hence, impact fretting wear and impact–sliding wear of cladding tube is needed to perform more research and evaluate reliability.
20/32
(a)Impact and tangential motion[110]
(b) Impact fretting[19]
Fig. 15 Impact and tangential motion of the cladding tube and impact fretting 4.5 Finite element analysis and numerical model on GTRF Finite element analysis (FEA) and numerical simulations have been used in GTRF to analyze the contact state, optimize spacer grid design, simulate vibration of the fuel rod, and predict wear rate. Yan [122] developed a method based on computational fluid dynamics to predict the GTRF in the fuel inlet region and found that a P-grid in fuel assembly inlet regions can greatly reduce the fretting damage. Bakosi [123] build an implicit large-eddy simulations of the time-dependent single-phase turbulent flow to calculate the shear forces with time on the fuel rods in 3 × 3 and 5 × 5 rod bundles with a single grid spacer. Kim [111–112, 124] used ANSYS to calculate the fuel rod vibration modes and natural frequencies and proposed that large initial elastic spring deflection of spacer grid, small cladding creep down, low spacer grid spring force relaxation, and large grid-to-rod contact area will reduce the fretting wear damage of cladding tube. Song [117] used a FEA to check a newly designed spacer grid and found that the new spacer grid can reduce the fretting wear of cladding tube and improve the crush strength of the spacer grid. Jiang [100, 125] proposed three-dimensional FEA models with detailed geometries of the dimple, spring, and fuel rods to evaluate the flow-induced impact intensity between the fuel rods and spacer grids. Mohany [126] developed a numerical model to predict the vibration response of CANDU fuel bundle and the associated fretting wear of cladding tube. This model discusses two excitation mechanisms, namely, turbulence-induced excitation and seismic excitation, and reveals that seismic excitation has no effect on the long-term fretting wear of fuel bundle. Blau [127–128] constructed a GTRF model based on the concepts of classical fretting to accommodate the complexities of the PWR environment. This empirical model can input the friction coefficient, slip amplitude, load history, frequency of oscillation, and contact area to determine the overall wear 21/32
depth and wear volume with time. Dyk [129] presented a modelling concept for the GTRF analysis of fuel rods caused by the vibration of coolant. Based on the simulated vibration model of the fuel rod, the evolution of the GTRF during operation can be determined. Lu [130–131] presented a numerical model combined with creep and wear to analyze the gap formation during grid-to-rod fretting and discussed the effect of pressure fluctuations, friction coefficients, wear coefficients, and initial interference on the wear profile and time at which contact is lost between the rod and grid. FEA and numerical simulation are important to analyze and predict the contact stress, vibration frequency, displacement amplitude, wear rate, and service life of cladding tube in PWR because GTRF in high-pressure water environment can hardly be monitored in actual condition and simulated in experimental conditions. FEA and numerical simulation are helpful to life prediction with engineering data, and they are key research points in the future. 4.6 Surface engineering technology applied on cladding tube To further satisfy the severe operation condition and improve the ability of accident tolerance, surface engineering is one of the most promising and effective ways to improve the property of cladding materials [132]. Three main principles for the selection of coating on zirconium alloy was proposed: (a) satisfy the operating conditions in the reactor and has a good corrosion resistance, hydrogen absorption resistance, radiation resistance, low thermal neutron capture cross section, and high heat transfer efficiency under normal operating conditions; (b) has an excellent ability of accident tolerance and good resistance to steam oxidation and thermal shock; and (c) has a good compatibility with zirconium alloy, such as expansion coefficient and preparation process [133]. The preparation methods of surface coating materials for zirconium alloys have been mainly reported in vapor deposition [134], cold spraying [135], micro-arc oxidation [136–137], thermal spraying [138], arc ion plating [139], and magnetron sputtering [140]. The studied coatings include the MAX phases (Ti2AlC [135], Ti3SiC2 [141]), carbide (SiC [134], ZrC [142]), nitride (TiN [143– 144]), oxide (ZrO2 [82, 136, 137], Al2O3 [145]), metal coating (FeCrAl [7, 146], Cr [87,148–149], Zr [149], and composite coating [150]). The preparation methods and properties of zirconium alloy surface coatings are shown in Table 5. Cr coating is the most promising coating for zirconium alloys due to its excellent high-temperature oxidation resistance [151]. Researchers are working on new coatings for zirconium alloys. At present, the selection of coating materials and coating process on zirconium alloys is a complicated process, which needs to be repeatedly verified in accordance with the research results of the key application properties of the coating, and a lot of research work is needed. 22/32
Table 5. Types and preparation process of coatings on the cladding tube Coating
Coating/Substrate
Coating process
Ti2AlC/Zr-4
Cold spraying
90
[135]
Ti3SiC2/Zr-4
Hot press
50-100
[141]
SiC/Zr-4
Chemical vapor deposition
1
[134]
ZrC/Zr-4
Chemical vapor deposition
-
[142]
TiN/ Zirlo
Physical vapor deposition
10
[143]
ZrO2/Zr-4, Zirlo, Zr-1Nb
Micro-arc oxidation
5-10
Al2O3/Zirlo
Atomic layer deposition
0.75
[145]
FeCrAl/ Zr alloys
Hot isostatic pressing
2
[146]
Cr/Zr-4
arc ion plated
10
[139]
FeCrAl, Zr /Mo
Physical vapor deposition
50
[149]
Cr-Zr /Cr/ Cr-N/E110, Zr-1Nb
Vacuum-arc evaporation
2
[150]
thickness/µm
Ref.
[82,136] [137]
4.7 Development trend of the fretting wear of cladding tube in the future GTRF has been studied for more than half a century ago, and cladding materials are constantly changing to improve the ability of accident tolerance. At present, key research points of GTRF should be focused on the following: (a) The development of new ATF cladding materials (coatings and alloy) is needed urgently to reduce the wear damage of GTRF. (b) More advanced techlonogies should be applied to the fretting wear test rig to similate high-radiation, high-pressure, and high-temperature water condition in reactors and monitor the state data and run region in real time. (c) More attention should be given to the failure mode of impact and impact–sliding wear on the cladding tube, which shows a more severe damage than the single tangential fretting wear. (d) Theoretical analysis should be emphasized to analyze the vibration state and predict the service life of the cladding tube combined with engineering and experimental data.
Conclusion Efforts to improve the existing research on impact fretting in nuclear power plants have been extensively reviewed in the present paper. The highlighted points are listed below: (a) Fretting wear equipment of various modes has been developed, and the test environment is becoming more similar to engineering practice. The contents of 23/32
fretting wear (e.g., materials, test conditions) are more than those of fatigue and corrosion (b)The fretting characteristics of advanced surface engineering technology applied to nuclear power plants is a research hotspot in the future. (c)As the nuclear power service environment is very complex, studying the damage progress of related materials under micro-action, obtaining real-time data, and carrying out life prediction are worthwhile.
Acknowledgement Young Scientific Innovation Team of Science and Technology of Sichuan (Nos. 2017TD0017) and National Natural Science Foundation of China (Nos.51627806) .
Reference [1]Pioro IL , Duffey R B , Kirillov P L, et al. Introduction: a survey of the status of electricity generation in the world. Handbook of Generation IV Nuclear Reactors, Elsevier, 2016 [2] Petroleum B . BP Statistical Review of World Energy - June 2019. Economic Policy, 2019, 6. [3]Mayuresh V K, Member A, Bernard M, et al., Level control in the steam generator of a nuclear power plant. IEEE T Contr Syst T 2000;8:55-69. [4]Zinkle S J, Was G S. Materials challenges in nuclear energy. Acta Mater 2013; 61: 735-758. [5]Kaczorowski D, Vernot J P. Wear problems in nuclear industry.Trib Int 2006:1286–1293. [6]Amanov A, Umarov R. The effects of ultrasonic nanocrystal surface modification temperature on the mechanical properties and fretting wear resistance of Inconel 690 alloy. Appl Surf Sci 2018;441:515-529. [7]Pernice M . Considerations for sensitivity analysis, uncertainty quantification, and data assimilation for grid-to-rod fretting. Office of Scientific & Technical Information Technical Reports, 2012. [8]Lu R Y , Karoutas Z , Sham T L . CASL virtual reactor predictive simulation: Grid-to-Rod Fretting wear. JOM 2011;63:53-58. [9]Blau P J. A multi-stage wear model for grid-to-rod fretting of nuclear fuel rods. Wear 2014; 313: 89-96. [10]Lee Y H , Kim H K, Kim H D, et al. A comparative study on the fretting wear of steam generator tubes in Korean power plants. Wear 2003;255:1198–1208. [11]Kim D G, Lee Y Z. Experimental investigation on sliding and fretting wear of steam generator tube materials. Wear 2001;250: 673–680. 24/32
[12] Mi X, Wang W X, Xiong X M, et al., Investigation of fretting wear behavior of Inconel 690 alloy in tube/plate contact configuration. Wear 2015;328: 582-590. [13]Mi X, Cai Z B, Xiong X M, et al., Investigation on fretting wear behavior of 690 alloy in water under various temperatures. Tribol Int 2016;100: 400-409. [14]Chung I L, Lee M H. An experimental study on fretting wear behavior of cross-contacting Inconel 690 tubes. Nucl Eng Des 2011;241: 4103–4110. [15] Ming H L, Liu X C, Zhang Z M, et al.Effect of normal force on the fretting wear behavior of Inconel 690 TT against 304 stainless steel in simulated secondary water of pressurized water reactor. Tribol Int 2018; 126: 133–143. [16] Attia M H , Magel E. Experimental investigation of long-term fretting wear of multi-span steam generator tubes with U-bend sections. Wear 1999;225–229 :563– 574. [17] Marc E, Fouvry S, Graton O, et al. Fretting wear of a nitride 316L/304L contact subject to in-phase normal force fluctuation in dry and lithium-boron solution: An RP-friction energy wear approach. Wear 2017;376-377:690–704. [18] Cai Z B, Peng J F, Qian H ,et al. Impact fretting wear behavior of alloy 690 tubes in dry and deionized water conditions. Chin J Mech Eng-En 2017:30: 819-828. [19]Lin Y W, Cai Z B,Chen Z Q, et al. Effect of diameter thickness ratio on alloy Zr-4 tube under impact fretting. Mater Today Comm, 2016;8:79–90. [20]Cai Z B,Chen Z Q, Sun Y,et al. Development of a novel cycling impact– sliding wear rig to investigate the complex friction motion. Friction 2019;7:32-43 [21]Soria S R, Tolley A, Yawny A.A study of debris and wear damage resulting from fretting of Incoloy 800 steam generator tubes against AISI Type 304 stainless steel. Wear 2016;368-369:219–229. [22] Kwon J D, Park D K, Woo S W, et al.A study on fretting fatigue life for the Inconel alloy 600 at high temperature. Nucl Eng and Des 2010; 240 :2521–2527 [23] Lgried M, Liskiewicz T, Neville A. Electrochemical investigation of corrosion and wear interactions under fretting conditions. Wear 2012;282-283: 52-58 [24]Guo X L, Lai P, Tang L C, et al., Fretting wear of alloy 690 tube mated with different materials in high temperature water. Wear 2018;400:119-126. [25] Guo X L, Lai P, Tang L C, et al. Time-dependent wear behavior of alloy 690 tubes fretted against 405 stainless steel in high-temperature argon and water. Wear 2018;414:194-201. [26] Lai P, Guo X L, Tang L C, et al. Effect of temperature on fretting wear behavior and mechanism of alloy 690 in water. Nucl Eng Des 2018; 327:51-60. [27] Do H H, Myung S C, Deok H L, et al. A case study on detection and sizing of defects in steam generator tubes using eddy current testing. Nucl Eng Des 2010; 240:204-208. 25/32
[28] Wu S B, Passivity degradation mechanism of steam generator alloys of PWRs in sulfur-containing environment, Master Thesis, Tianjin University, Tianjin, China, 2018. [29] Li J, The fretting wear behavior and damage mechanism of heat exchange tube materials in air and solution environments, Ph.D. Thesis, University of Science and Technology Beijing, Beijing, China, 2017. [30] Zhang X Y, Studies on tangential fretting wear mechanisms of steam generator tubes in nuclear power systems, Ph.D. Thesis, Southwest Jiaotong University, Chengdu, China, 2013. [31] Xin L, Fretting wear behavior and damage mechanism of nuclear grade Inconel 690 TT alloy, Ph.D. Thesis, University of Science and Technology Beijing, Beijing, China, 2018. [32] Lake J A, The fourth generation of nuclear power. Prog Nucl Energy 2002;40:301-307. [33] Marques J G. Evolution of nuclear fission reactors: Third generation and beyond. Energ Convers Manage 2010;51:1774-1780. [34] Horvath A, Rachlew E, Nuclear power in the 21st century: Challenges and possibilities. Ambio, 2016;45:38-49. [35] Kissane M P, A review of radionuclide behaviour in the primary system of a very-high-temperature reactor. Nucl Eng Des 2009;239:3076-3091. [36] Klueh R L, Nelson A T. Ferritic/martensitic steels for next-generation reactors. J Nucl Mater 2007;371:37-52. [37] Glasstone S, Sesonske A, Nuclear reactor engineering: reactor systems engineering. Springer Science & Business Media, 2012. [38] Connors H J. Flow-induced vibration and wear of steam generator tubes. Nucl Technol 1981; 55:311-331. [39] Li J, Lu Y H, Effects of displacement amplitude on fretting wear behaviors and mechanism of Inconel 600 alloy. Wear 2013;304: 223-230. [40] Xin L, Wang Z H, Li J, et al. Fretting wear behavior and mechanism of Inconel 690 alloy related to the displacement amplitude. Tribol T 2017;60: 913-922. [41] Soria S R, Tolley A, Yawny A, A study of debris and wear damage resulting from fretting of Incoloy 800 steam generator tubes against AISI Type 304 stainless steel. Wear 2016;368: 219-229. [42] Yun J Y,Park M C, Shin G S, et al., Effects of amplitude and frequency on the wear mode change of Inconel 690 SG tube mated with SUS 409. Wear 2014;313:83-88. [43] Li J, Ma M, Lu Y H, et al. Evolution of wear damage in Inconel 600 alloy due to fretting against type 304 stainless steel. Wear 2016;346:15-21. 26/32
[44] Xin L, Lu Y H, Shoji T. The role of material transfer in fretting wear behavior and mechanism of Alloy 690TT mated with Type 304 stainless steel. Mater Charact 2017; 130 :250-259. [45] Li J, Yang B B, Lu Y H, et al., The degradation mechanism of Inconel 690TT induced by fretting wear in air. Tribol Int 2017;116:147-154. [46] Soria S A, Tolley A, Yawny A, Characterization of damage and triboparticles resulting from fretting of incoloy 800 steam generator tubes against different materials. Wear 2017; 390:198-208. [47] Xin L, Yang B B, Wang Z H, et al., Microstructural evolution of subsurface on Inconel 690TT alloy subjected to fretting wear at elevated temperature. Mater Des 2016;104:152-161. [48] Xin L, Yang B B, Li J, et al. Wear damage of Alloy 690TT in partial and gross slip fretting regimes at high temperature. Wear 2017; 390:71-79. [49] Xin L, Lu Y H, Shoji T. The comparative study on nanostructured tribolayers of Alloy 690TT subjected to fretting wear under different oxygen contents. Mater Charact 2017;131:157-167. [50] Zhang X Y, Liu J H, Cai Z B, et al., Experimental study of the fretting wear behavior of Incoloy 800 alloy at high temperature. Tribol T 2017; 60:1110-1119. [51] Zhang X Y, Cai Z B, Peng J F,et al. Experimental study of the fretting wear behavior of Inconel 690 alloy under alternating load conditions. Proc IMechE Part J:J Eng Tribol 2018;232:1343–1351 [52] Xin L, Ma M, Lu Y H, et al. Comparative study on fretting wear behaviors of Alloy 600MA in dry air and deionized water conditions. Wear 2019;418:167-179. [53] Li J, Yang B B, Lu Y H, et al. The effects of electrochemical polarization condition and applied potential on tribocorrosion behaviors of Inconel 690 alloys in water environment. Mater Des 2017;119:93-103. [54] Xin L, Yang B B, Wang Z H, et al., Effect of normal force on fretting wear behavior and mechanism of Alloy 690TT in high temperature water. Wear 2016; 368:210-218 [55] Guo X L, Lai P, Tang L C, et al., Effects of sliding amplitude and normal load on the fretting wear behavior of alloy 690 tube exposed to high temperature water. Tribol Int 2017; 116:155-163. [56] Liao J, Wu X, Tan J, et al., Fretting corrosion fatigue of Alloy 690 in high-temperature pure water. Corros Sci 2018; 133 :423-431. [57] Xin L, Lu Y H, Otsuka Y, et al., The role of frequency on fretting corrosion of Alloy 690TT against 304 stainless steel in high temperature high pressure water. Mater Charact 2017;134 :260-273. [58] Wang Z H, Lu Y H, Li J, et al., Effect of pH value on the fretting wear 27/32
behavior of Inconel 690 alloy. Tribol Int 2016; 95:162-169. [59] J. Li J, B. Yang B, Y. Lu Y H, et al., The effect of normal force on fretting corrosion behavior of Inconel 690 in 3.5% sodium chloride. M Mater. Charact 2017;., 131:224-233. [60] Guan H D, Cai Z B, Ren Y P, et al., Impact-fretting wear behavior of Inconel 690 alloy tubes effected by pre-compressive stress. J Alloy Compd 2017; 724:910-920. [61] Sun Y, Cai Z B, Chen Z Q, et al. Impact fretting wear of Inconel 690 tube with different supporting structure under cycling low kinetic energy. Wear 2017;376:625-633. [62] Cai Z B, Chen Z Q,Qian H, et al., Impact fretting wear behavior of 304 stainless steel thin-walled tubes under low-velocity. Tribol Int 2017; 105:219-228. [63] Souilliart T,Rigaud E, Bot A L, Energy-based wear law for oblique impacts in dry environment. Tribol Int 2017; 105: 241-249. [64] Souilliart T, Rigaud E, Bot A L, et al., An energy approach for impact wear in water environment. Wear 2017;376: 738-746. [65] Yin M G, Cai Z B, Zhang Z X, et al. Effect of ultrasonic surface rolling process on impact-sliding wear behavior of the 690 alloy. Tribol Int (2019). doi:https://doi.org/10.106/j.triboint.2019.02.008. [66]Chen Z Q. Development of the impact-sliding wear test rig and experimental research, Master Thesis, Southwest Jiaotong University, Chengdu, China, 2017. [67] Yin M G, Ca i Z B, Yu Y Q, Zhu M H.Impact-sliding wear behaviors of 304SS influenced by different impact kinetic energy and sliding velocity.Tribol Int 10.1016/j.triboint.2019.106057. [68] Wang Z, Lu Y H, Zhang H Y, et al. Effect of cold rolling on the fretting wear behavior and mechanism in Inconel 600 alloy. Tribol T 2016;59:923-931. [69] Li J, Lu Y H, Zhang H Y, et al., Effect of grain size and hardness on fretting wear behavior of Inconel 600 alloys. Tribol Int 2015;81:215-222. [70] Lee T H , Suh H Y, Han S K, et al., Effect of a heat treatment on the precipitation behavior and tensile properties of alloy 690 steam generator tubes. J Nucl Mater 2016;479:85-92. [71] Zhang H Y, Lu Y H, Ma M, et al., Effect of precipitated carbides on the fretting wear behavior of Inconel 600 alloy. Wear 2014;315:58-67 [72] Li K, He Y, Cho I S, et al., Effect of ultrasonic nanocrytalline surface modification on the microstructural evolution of Inconel 690 alloy. Mater Manuf Process 2015; 30:194-198. [73] D'Agata E, Hania P R, Freis D, et al. The MARINE experiment: Irradiation of sphere-pac fuel and pellets of UO2− x for americium breading blanket concept . Nucl Eng Des 2017;311: 131-141. 28/32
[74] Björk K I, Kelly J F, Vitanza C, et al. Irradiation testing of enhanced uranium oxide fuels . Ann Nucl Energ 2019;125: 99-106. [75] Arlit M, Partmann C, Schleicher E, et al. Instrumentation for experiments on a fuel element mock-up for the study of thermal hydraulics for loss of cooling or coolant scenarios in spent fuel pools. Nucl Eng Des 2018;336:105-111. [76] Kim K T. Evolutionary developments of advanced PWR nuclear fuels and cladding materials. Nucl Eng Des 2013; 263:59-69. [77] Kim H K. Mechanical analysis of fuel fretting problem. Nucl Eng Des 1999; 192:81-93. [78] Liu H D, Chen D Q, Hu L, et al. Numerical investigations on flow-induced vibration of fuel rods with spacer grids subjected to turbulent flow. Nucl Eng Des 2017; 325: 68-77. [79] Lewis B J, El-Jaby A, Higgs J, et al. A model for predicting coolant activity behaviour for fuel-failure monitoring analysis. J Nucl Mater 2007; 366: 37-51. [80] Kim H K, Lee Y H, Lee K H. On the geometry of the fuel rod supports concerning a fretting wear failure. Nucl Engin Des 2008;238: 3321-3330. [81] Zhou B F, Feng K Q. Zr–Cu alloy filler metal for brazing SiC ceramic. RSC Adv 2018;8: 26251-26254. [82] Wei K J , Chen L , Qu Y , et al. Zeta potential of microarc oxidation film on zirlo alloy in different aqueous solutions . Corros Sci 2018;143:129-135. [83] Zhou J , Li Z K . Research progress on cladding materials used for light water reactor. Mater China, 2014;33:554-559. [84] Pint B A, Terrani K A, Yamamoto Y, et al. Material selection for accident tolerant fuel cladding . Metall Mater Trans E, 2015;2:190-196. [85] Massey C P, Terrani K A, Dryepondt S N, et al. Cladding burst behavior of Fe-based alloys under LOCA. J Nucl Mater 2016;470: 128-138. [86] Gerasimov V V, Monakhov A S. Corrosion of reactor materials. 1994. [87] Kim H G, Kim I H, Jung Y I, et al. Adhesion property and high-temperature oxidation behavior of Cr-coated Zircaloy-4 cladding tube prepared by 3D laser coating. J Nucl Mater 2015;465:531-539. [88] Zhao W J, Liu Y Z, Jiang H M, et al. Effect of heat treatment and Nb and H contents on the phase transformation of N18 and N36 zirconium alloys. J Alloy Compd, 2008;462: 103-108. [89] Mardon J P, Charquet D, Senevat J. Influence of composition and fabrication process on out-of-pile and in-pile properties of M5 alloy[C]//Zirconium in the Nuclear Industry: Twelfth International Symposium. ASTM International, 2000. [90] Terrani K A. Accident tolerant fuel cladding development: Promise, status, and challenges. J Nucl Mater 2018;501: 13-30. 29/32
[91] Zinkle S J, Terrani K A, Gehin J C, et al. Accident tolerant fuels for LWRs: A perspective . J Nucl Mater 2014;448: 374-379. [92] Cho K H, Kim T H, Kim S S. Fretting wear characteristics of Zircaloy-4 tube. Wear 1998; 219: 3-7. [93] Kim T H, Kim S S. Fretting wear mechanisms of Zircaloy-4 and Inconel 600 contact in air. KSME Int J 2001;15: 1274-1280. [94] Attia M H. On the fretting wear mechanism of Zr-alloys. Tribol Int, 2006;39: 1320-1326. [95] Attia M H . Fretting wear of Zr-alloy pressure tubes under the combined effects of in-plane and out-of-plane flow-induced vibrations. Wear 2005;259:319-328. [96] Winter T C, Neu R W, Singh P M, et al. Fretting wear comparison of cladding materials for reactor fuel cladding application. J Nucl Mater 2018;508: 505-515. [97] Winter T, Neu R W, Singh P M, et al. Coefficient of friction evolution with temperature under fretting wear for FeCrAl fuel cladding candidate. J Nucl Mater 2019;520: 140-151. [98] Lazarevic S, Lu R Y, Favede C, et al. Investigating grid-to-rod fretting wear of nuclear fuel claddings using a unique autoclave fretting rig. Wear 2018;412: 30-37. [99] Qu J, Cooley K M, Shaw A H, et al. Assessment of wear coefficients of nuclear zirconium claddings without and with pre-oxidation. Wear 2016;356: 17-22. [100] Jiang H, Qu J, Lu R Y, et al. Grid-to-rod flow-induced impact study for PWR fuel in reactor. Prog Nucl Energ 2016;91: 355-361. [101] Zhang L F, Lai P, Liu Q D, et al. Fretting wear behavior of zirconium alloy in B-Li water at 300° C. J Nucl Mater 2018;499: 401-409. [102] Lai P, Zhang H, Zhang L F, et al. Effect of micro-arc oxidation on fretting wear behavior of zirconium alloy exposed to high temperature water. Wear 2019;424: 53-61. [103] Lucadamo G A, Howland W H, Tymiak-Carlson N, et al. Characterization and simulation methods applied to the study of fretting wear in Zircaloy-4. Wear 2018; 402: 11-20. [104] Lee Y H, Kim H K. Effect of spring shapes on the variation of loading conditions and the wear behaviour of the nuclear fuel rod during fretting wear tests. Wear 2007; 263: 451-457. [105] Lee Y H, Kim H K. Evaluation of fretting wear behavior on the simulated supporting structures of a dual-cooled nuclear fuel rod[C]//Materials Science Forum. Trans Tech Publications, 2010, 654: 2564-2567. [106] Lee Y H, Kim H K. Fretting wear behavior of a nuclear fuel rod under a simulated primary coolant condition. Wear 2013;301: 569-574. 30/32
[107] Lee Y H, Kim H K, Kang H S, et al. Fretting wear behaviors of a dual-cooled nuclear fuel rod under a simulated rod vibration[C]//AIP Conference Proceedings. AIP, 2012, 1448: 235-241. [108] Kim H K, Lee Y H. Influence of contact shape and supporting condition on tube fretting wear. Wear 2003;255: 1183-1197. [109] Kim H K, Lee Y H, Heo S P. Mechanical and experimental investigation on nuclear fuel fretting. Tribol Int 2006;39:1305-1319. [110] Kim H K, Kim S J, Yoon K H, et al. Fretting wear of laterally supported tube. Wear 2001;250: 535-543. [111] Kim K T, Suh J M. Impact of nuclear fuel assembly design on grid-to-rod fretting wear. J Nucl Sci Technol 2009 46:149-157. [112] Kim K T. Applicability of out-of-pile fretting wear tests to in-reactor fretting wear-induced failure time prediction. J Nucl Mater 2013;433: 364-371. [113] Hu Z P. Developments of analyses on grid-to-rod fretting problems in pressurized water reactors. Prog Nucl Energ 2018;106: 293-299. [114] Hu Z P, Thouless M D, Lu W. Effects of gap size and excitation frequency on the vibrational behavior and wear rate of fuel rods. Nucl Eng Des 2016;308: 261-268. [115] Kovács S, Stabel J, Ren M, et al. Comparative study on rod fretting behavior of different spacer spring geometries. Wear 2009;266: 194-199. [116] Shin M K, Lee H A, Lee J J, et al. Optimization of a nuclear fuel spacer grid spring using homology constraints. Nucl Eng Des 2008;238: 2624-2634. [117] Song K N, Lee S B, Shin M K, et al. New spacer grid to enhance mechanical/ structural performance. J Nucl Sci Technol 2010;47: 295-303. [118] Rubiolo P R. Probabilistic prediction of fretting-wear damage of nuclear fuel rods. Nucl Eng Des 2006; 236:1628-1640. [119] Ko P L. Wear of zirconium alloys due to fretting and periodic impacting. Wear 1979;55: 369-384. [120] Jones D H, Nehru A Y, Skinner J. The impact fretting wear of a nuclear reactor component. Wear;1985, 106: 139-162. [121] Fisher N J, Weckwerth M K , Grandison D A E, et al. Fretting-wear of zirconium alloys . Nucl Eng Des 2002; 213:79-90 [122] Yan J, Yuan K, Tatli E, et al. A new method to predict Grid-To-Rod Fretting in a PWR fuel assembly inlet region. Nucl Eng Des 2011;241: 2974-2982. [123] Bakosi J, Christon M A , Lowrie R B , et al. Large-eddy simulations of turbulent flow for grid-to-rod fretting in nuclear reactors . Nucl Eng Des 2013; 262:544-561. [124] Kim K T. The effect of fuel rod supporting conditions on fuel rod vibration 31/32
characteristics and grid-to-rod fretting wear. Nucl Eng Des 2010;240: 1386-1391. [125] Jiang H, Wang J A J, Wang H. The impact of interface bonding efficiency on high-burnup spent nuclear fuel dynamic performance. Nucl Eng Des 2016;309: 40-52. [126] Mohany A , Hassan M . Modelling of fuel bundle vibration and the associated fretting wear in a CANDU fuel channel. Nucl Eng Des 2013; 264:214-222. [127] Blau P J, Qu J, Lu R. Modeling of complex wear behavior associated with grid-to-rod fretting in light water nuclear reactors. JOM 2016;68: 2938-2943. [128] Blau P J. A microstructure-based wear model for grid-to-rod fretting of clad nuclear fuel rods. Wear 2019;426: 750-759. [129] Dyk Š, Zeman V. Evolution of grid-to-rod fretting of nuclear fuel rods during burnup. Prog Nucl Energ 2018;108: 160-168. [130] Wang H, Hu Z P, Lu W, et al. The effect of coupled wear and creep during grid-to-rod fretting. Nucl Eng Des 2017;318: 163-173. [131] Lu W, Thouless M D, Hu Z P, et al. CASL structural mechanics modeling of grid-to-rod fretting (GTRF) . JOM 2016;68: 2922-2929. [132] Cheng T, Keiser J R, Brady M P, et al. Oxidation of fuel cladding candidate materials in steam environments at high temperature and pressure. J Nucl Mater 2012;427: 396-400. [133] Bai G H, Chen Z L, Zhang Y W, et al. Research progress of coating on zirconium alloy for nuclear fuel cladding. Rare Metal Mat Eng 2017;46: 2035-2040. [134] Al-Olayyan Y, Fuchs G E, Baney R, et al. The effect of Zircaloy-4 substrate surface condition on the adhesion strength and corrosion of SiC coatings. J Nucl Mater 2005;346: 109-119. [135] Maier B R, Garcia-Diaz B L, Hauch B, et al. Cold spray deposition of Ti2AlC coatings for improved nuclear fuel cladding. J Nucl Mater 2015;466: 712-717. [136] Wang Y M, Feng W, Xing Y R, et al. Degradation and structure evolution in corrosive LiOH solution of microarc oxidation coated Zircaloy-4 alloy in silicate and phosphate electrolytes. Appl Surf Sci 2018;431: 2-12. [137] Yang J X, Wang X, Wen Q, et al. The effect of microarc oxidation and excimer laser processing on the microstructure and corrosion resistance of Zr–1Nb alloy . J Nucl Mater 2015;467: 186-193. [138] Jin D, Yang F, Zou Z, et al. A study of the zirconium alloy protection by Cr3C2–NiCr coating for nuclear reactor application. Surf Coat Tech 2016;287: 55-60. [139] Park J H, Kim H G, Park J, et al. High temperature steam-oxidation behavior of arc ion plated Cr coatings for accident tolerant fuel claddings. Surf Coat Tech 2015; 280: 256-259. 32/32
[140] Zhong W, Mouche P A, Han X, et al. Performance of iron–chromium– aluminum alloy surface coatings on Zircaloy 2 under high-temperature steam and normal BWR operating conditions. J Nucl Mater 2015;470:327-338. [141] Tallman D J, Yang J, Pan L, et al. Reactivity of Zircaloy-4 with Ti3SiC2 and Ti2AlC in the 1100–1300° C temperature range. J Nucl Mater 2015;460: 122-129. [142] Katoh Y, Vasudevamurthy G, Nozawa T, et al. Properties of zirconium carbide for nuclear fuel applications. J Nucl Mater 2013;441: 718-742. [143] Alat E, Motta A T, Comstock R J, et al. Multilayer (TiN, TiAlN) ceramic coatings for nuclear fuel cladding. J Nucl Mater 2016;478: 236-244. [144] Sung J H, Kim T H, Kim S S. Fretting damage of TiN coated zircaloy-4 tube . Wear 2001;250: 658-664. [145] Lorenzo-Martin C, Ajayi O O, Hartman K, et al. Effect of Al2O3 coating on fretting wear performance of Zr alloy. Wear 2019;426: 219-227. [146] Terrani K A, Zinkle S J, Snead L L. Advanced oxidation-resistant iron-based alloys for LWR fuel cladding. J Nucl Mater 2014;448: 420-435. [147] Maier B, Yeom H, Johnson G, et al. Development of cold spray coatings for accident-tolerant fuel cladding in light water reactors. JOM 2018;70: 198-202. [148] Park D J, Kim H G, Jung Y I, et al. Behavior of an improved Zr fuel cladding with oxidation resistant coating under loss-of-coolant accident conditions. J Nucl Mater 2016;482: 75-82. [149] Cheng B, Kim Y J, Chou P. Improving accident tolerance of nuclear fuel with coated Mo-alloy cladding. Nucl Eng Tech 2016;48: 16-25. [150] Kuprin А S, Belous VА, Voyevodin V N, et al. Vacuum-arc chromium-based coatings for protection of zirconium alloys from the high-temperature oxidation in air . J Nucl Mater 2015;465:400-406. [151] Idarraga-Trujillo I, Le Flem M, Brachet J C, et al. Assessment at CEA of coated nuclear fuel cladding for LWRs with increased margins in LOCA and beyond LOCA conditions. LWR Fuel Performance Meeting 2013.
33/32
Table 2. Fourth-generation nuclear reactors and their materials in heat exchange Type
Thermal Neutron Reactors
Fast Neutron Reactors
Reactor
Coolant
Coolant temperature In/out( )
Materials for heat exchanger
Supercritical water reactor
Light-water
280 (inlet)/500 (o utlet)
Very high temperature reactor
Helium
640 (inlet)/≥950 ( outlet)
Martensitic/ Ferrite Stainless Steel/ Austenite Steel Nickel Base Alloy/ Ceramic
Liquid salt
565 (inlet)/≥700 ( outlet) 490 (inlet)/≥850 ( outlet)
Gas-cooled Fast reactor
Helium
Sodium-coole d fast reactor
Liquid sodium
98 (inlet)/≥550 (o utlet)
Lead-cooled fast reactor
Molten lead or lead-bismuth eutectic
420 (inlet)/≥540 ( outlet)
Nickel Base Alloy Martensitic/ Ferrite Stainless Steel/ Austenite Steel/ Oxide Dispersion-Strengthened Alloy/ Nickel Base Alloy/ Ceramic Martensitic/ Ferrite Stainless Steel/ Austenite Steel/ Oxide Dispersion-Strengthened Alloy Martensitic/ Ferrite Stainless Steel/ Austenite Steel/ Oxide Dispersion-Strengthened Alloy
Highlights
1.
The research status of fretting method, nuclear materials damage in key equipment and structures of nuclear power plant is reviewed.
2.
Fretting research of heat exchange materials for steam generators in nuclear power systems is reviewed.
3.
The research status of fretting wear of fuel cladding is analyzed, including the latest coating and surface strengthening technologies.