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Advances in Materials Science and Engineering
Volume 2014 (2014), Article ID 791462, 6 pages
Wear Behaviour of Nanocrystalline Fe88Si12 Alloy in Water Environment
State Key Laboratory of Solid Lubrication, Lanzhou Institute of Chemical Physics, Chinese Academy of Sciences, Lanzhou 730000, China
Received 2 May 2013; Accepted 15 October 2013; Published 6 January 2014
Academic Editor: Pavel Lejcek
Copyright © 2014 Licai Fu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Wear behaviour of nanocrystalline Fe88Si12 alloy has been investigated in water environment compared with the coarse grained counterpart. The friction coefficient of the Fe88Si12 alloy changes slightly with the grain size. The wear resistance is enhanced as the grain size decreases first and then reduces when the grain size continues to decrease, although the hardness of the Fe88Si12 alloy decreases monotonically with the grain size. It is contrary to the predications of Archard’s formula. The best wear resistance of Fe88Si12 alloy with grain size of 40 nm in our present work is attributed to the proper grain boundary volume fraction and composite phase structures of disordered B2 and ordered D03.
In recent decades, how to improve the wear resistance of engineering materials with lubricant has received much attention. Fretting is often an origin of catastrophic failures or loss of functionality in many engineering applications, such as bolted mechanical joints, stacks of objects in transport, and electrical connectors in vibrating machinery and so on. Lots of researchers tried to develop novel wear resistance materials for application in water environment because of pollution caused by oil hydraulic systems [1–3]. Since water has low viscosity and poor lubricity, many conventional materials used in oil hydraulics cannot be used in water condition.
The nanocrystalline materials are of great scientific importance because of the small grain size and significant grain boundaries (GB) volume fraction. Correspondingly, their physical and chemical properties, which are highly sensitive to their microstructure, suggest various potential structure and engineering applications [4–6]. The friction and wear properties of the nanocrystalline materials also have received considerable interest due to the high hardness compared with the coarse grained counterparts [7–10]. Takagi et al. , Jeong et al. , and Han et al.  indicated that the friction coefficient and wear rate of the nanostructured metals and alloys were not only decided by grain size, but also influenced by morphology, phase structure. Although some studies had been undertaken to investigate the tribological behaviour of the nanocrystalline metals and alloys, there seem to be only a few reports on the tribological properties of the nanocrystalline metals and alloys in water condition.
In the present work, the wear behaviour of the bulk nanocrystalline alloy, which was successfully prepared by combustion synthesis technique , was comparatively studied using a conventional tribological tester in water environment.
2. Experimental Procedures
The alloy has been prepared by combustion synthesis technique . Different grain sizes of the alloy were obtained by annealing at different temperatures in air. The grain sizes of the prepared and annealed alloy are 10 nm, 20 nm, 40 nm, and 30 m, which were designated as , , , and CG, respectively. The hardness increases monotonically with the grain size. According to statistics of XRD and TEM images and corresponding selected area electronic diffraction patterns, the phase structures of the alloys are shown in Table 1. CG is fully composed of relative disordered B2 structure. The phase structure changes from relative disordered B2 to ordered when the grain size decreases. And the B2 structure is only about 9 at.% for . The GB volume fractions were calculated by equation , where is width of GB and is grain size. In this case, we supposed that is 1 nm. The GB volume fraction dramatically increases as the grain size decreases to nanoscale size (Table 1). In particular, the GB volume fraction of is about eighth of total volume of alloys. The relative ordered phase structure and the huge GB volume fraction would affect the properties of alloy with nanoscale size.
The wear behaviour of the alloys was evaluated on an Optimol SRV oscillating friction and wear tester at room temperature (about 25°C) and humidity of 30% in water environment. The surfaces of the discs were polished with 600-grit SiC emery paper. The counterpart is a Si3N4 ceramic ball with a diameter of 9.53 mm, Vicker’s microhardness of 19 GPa, and surface roughness of 0.01 m. The oscillating speed ranges from 0.02 to 0.08 m/s. The applied load is 30 N. The profiles of worn scars were measured using a micro-XAM surface mapping microscope to determine the wear volume . The wear rate was determined as , where is total sliding distance. At least three tests were conducted for each set of testing parameters and the average values were calculated from the data of the three tests. The relative error for the friction and wear tests was below 10%. Morphologies and compositions of the worn surfaces of the Fe88Si12 alloys at different wear conditions were examined by using a JSM-5600LV scanning electron microscope (SEM) and a PHI-5702 multifunctional X-ray photoelectron spectroscope (XPS). The XPS analysis was conducted at 400 W and a pass energy of 29.4 eV, using Al K radiation as the exciting source and the binding energy of contaminated carbon (C1s: 284.6) as the reference.
3. Results and Discussion
A representative curve of the evolution of friction coefficient of NC10 indicates that the friction coefficient becomes steady after the initial transient running time (inset of Figure 1(a)). The average friction coefficients in the steady state of all the Fe88Si12 alloys increase at a low speed and basically keep stable at high speed in error range (Figure 1(a)). The average friction coefficients of all the Fe88Si12 alloys with identical speed are very close. This means that the friction coefficient of the Fe88Si12 alloy changes slightly with grain size in water condition.
The wear rate of the Fe88Si12 alloy decreases as the grain size reduces to 40 nm (Figure 1(b)), while the wear rate increases when the grain size decreases from 40 nm to 10 nm. In other words, the Fe88Si12 alloy with grain size of 40 nm has the best wear resistance in water environment for these samples. However, the best wear resistance may occur with grain size of between 20 nm and 30 m, because limited grain sizes of the Fe88Si12 alloy have been examined in this paper. We will test the wear rate of this alloy with other grain sizes of follow-up studies. The wear resistance of the Fe88Si12 alloy with nanoscale grain size varied with the speed is opposite to CG. The wear rates of NC10, NC20, and NC40 increase at low speed and retain unchanged at high speed. On the contrary, the wear rate of CG decreases at low speed (Figure 1(b)). These facts demonstrate that the wear behaviour of the Fe88Si12 alloy markedly changes near the grain size of 40 nm.
The SEM micrographs show severe microgrooves and mild delamination on the worn surfaces of all the Fe88Si12 alloys at speed of 0.02 m/s (Figure 2). The wear mechanism of all the Fe88Si12 alloys is dominated by microgrooves and delamination at low speed. However, the plough on the worn surfaces of NC10, NC20, and NC40 becomes mild as speed increases, whereas the plough changes severely with increasing speed for CG. Some microcracks are observed on the worn surfaces of all the NC10, NC20, and NC40 under high speed. Severe delamination and some oxides can be found on the worn surface of CG.
Vickers’ microhardness of the Fe88Si12 alloy increases from 5.1 GPa to 10 GPa when the grain size decreases from 30 m to 10 nm. Generally, the wear loss is inversely proportional to the hardness of the material according to Archard’s equation . The high hardness indicates that lesser debris could detach from the sample. It restrains both crack propagation and wear fragments formation. So the wear resistance of the Fe88Si12 alloy should improve as the grain size decreases to 10 nm. However, it is difficult to depict why the NC40 just with hardness 5.3 GPa has better wear resistance in these samples. The previous researches indicated that tribological chemical reaction might play an important role in the dry wear, especially for nanocrystalline metals and alloys , because the interface of nanocrystalline metals and alloys has become an important structural component in addition to the grains, which results in producing some anomalous properties. For example, fast diffusion behaviour of nanocrystalline material has been reported . The tribological chemical reactions on the worn surfaces may be different for the Fe88Si12 alloys with different grain sizes. So, in this case, the chemical states on the worn surfaces of all the Fe88Si12 alloys have been investigated by XPS.
The Fe and Si XPS spectra of worn surfaces of the Fe88Si12 alloys are shown as in Figures 3 and 4. The Fe2p peaks including Fe2p3/2 and Fe2p1/2 peaks of all the Fe88Si12 alloys can be systematically decomposed into Fe2O3, FeO(OH), and Fe2SiO4 compounds on the basis of references data published elsewhere [18, 19]. An additional weak peak of Fe3O4 can be detected on the worn surface of CG. The intensity of both FeO(OH) and Fe2SiO4 peaks increases as the grain size increases from 10 nm to 40 nm and then markedly decreases when the grain size increases to 30 m. On the contrary, the strong Fe2p1/2 peak of Fe2O3 is observed on the worn surfaces of NC10, NC20, and CG, while it is not found on the worn surface of NC40. It demonstrates that FeO(OH) and Fe2SiO4 layers can be formed easier onto the worn surface of NC40 than other samples in water environment.
Similarly, the Si2p spectra of the Fe88Si12 alloys with nanoscale grain sizes can be divided into Fe2SiO4, Fe3Si, and SiO2 peaks (Figures 4(a), 4(b), and 4(c)) [19, 20]. However the SiO2 cannot be observed on the worn surface of CG (Figure 4(d)). The intensity of Fe2SiO4 peak decreases as the grain size increases, while it increases for Fe3Si. The Si3N4 may originate from the detached debris of the Si3N4 ball between contacted zones of friction pair and has not been fully oxidized on the worn surface of CG. According to the analysis of Figures 3 and 4, it is concluded that the Fe2SiO4, SiO2, and FeO(OH) composite films form easier on the worn surface of NC40 than NC10, NC20, and CG.
There are large numbers of high-energy defects in nanocrystalline metals and alloys, such as GB, microvoids, lattice distortion, crystal defect, and internal stress. The GB volume fraction increases from about 0.005 vol.% to 7.3 vol.% as the grain size reduces to 40 nm (Table 1). So Fe and Si elements in Fe-Si alloy with nanoscale grain size exhibit strong inclination to segregate to the defects . Meanwhile, a large amount of Si will accumulate on the worn surface of sample with small grain size because of the fast diffusion effect compared with CG. The accumulated Si is preferentially oxidized to form continuous SiO2 and Fe2SiO4 composite film in water environment, which significantly prevent further oxidation and wear.
On the other hand, the specific phase structure of Fe88Si12 alloys also influences the oxides formation on the surface of the Fe-Si alloy. Lots of reports indicated that the oxide behaviour of the Fe-Si alloy depended on the Si content. Low-Si alloys have a reducible Fe oxide layer, while Si-rich alloys form thick and stable SiO2 layers. For instance, Wolff et al. showed that the stable SiO2 layer formed on the surface of Fe-24 at.% Si alloy in borate solution . Atkinson  predicted that the Fe-Si alloy surface would form SiO2 and Fe2SiO4 films in water when the Si content was larger than 5 at.% Si, but form Fe3O4 with Fe2SiO4 films as the Si content was less than 5 at.%. As the Si content in Fe-Si alloy increases, three different phases of -Fe, Fe3Si, and FeSi form in turn. The ordered D03 Fe3Si easily forms Fe2SiO4 and SiO2 layers, and disordered B2 Fe(Si) generates Fe2O3, which transforms FeO(OH) in water environment. The phase structures of the Fe88Si12 alloy change from D03 and B2 to B2 as the grain size increases. The B2 structure almost disappears for NC10, which suggests that there should form few FeO(OH) and Fe2O3 on the worn surface of NC10 in the water environment. So the NC40 and NC20 with composite structure of D03 and B2 would be in favor of forming FeO(OH)/Fe2O3, SiO2, and Fe2SiO4 composite films. The Fe2SiO4 content on worn surface of NC20 is equivalent to NC10, which is less than NC40 (Figure 3). As GB volume fraction increase above 14.3% (Table 1), the oxidation films may become loose and easy to delaminate when lots of oxide form on the Fe-Si alloy worn surface. Thus, oxidation films on NC20 worn surface have been removed in wear. Thus, some of the composite films loosen on the worn surface of NC20 and have been removed in wear. However, the different phase structures of the Fe88Si12 alloy originate from the different grain sizes rather than with identical grain size. It is still difficult to judge which factor is playing more roles during wear. The relation of oxidation and disordered and ordered composite structures should be further examined in the future.
The above discussions demonstrate that the wear behaviour exhibited significantly different characters for the Fe88Si12 alloys with different grain sizes. The hardness of the Fe88Si12 alloy increases with decrease of the grain size. So the wear resistance of Fe88Si12 alloys with grain size of nanoscale is better than CG. The SEM and XPS of the worn surfaces of the Fe88Si12 alloys show that the tribochemistry reaction plays an important role during wear in water condition. The worn surface presents protected films and less microplough for NC40. Because the FeO(OH), Fe2SiO4, and SiO2 composite films form easier on the worn surface of the NC40 than other Fe88Si12 alloys, so the best wear resistance is obtained for the Fe88Si12 alloy with grain size of 40 nm in the present work.
(1)The friction coefficient of the Fe88Si12 alloy changes slightly with grain in water environment.(2)The hardness of the Fe88Si12 alloy increases with decrease of the grain size. The wear resistance of the Fe88Si12 alloy does not show monotonic improvement as the grain size decreases according to Archard’s equation, while it improves as the grain size decreases to 40 nm, and then decreases when the grain size continues to decrease to 10 nm.(3)The best wear resistance of the Fe88Si12 alloy with grain size of 40 nm in our present work is attributed to the specific microstructure. First, the high-energy interfaces of the Fe88Si12 alloy increase rapidly as the grain size decreases to nanoscale, which can improve the tribochemical reactions of the Fe88Si12 alloy in water environment. Second, the composite ordered D03 and disordered B2 structures are beneficial to forming Fe2SiO4 and FeO(OH) composite films. It possesses excellent wear resistance comparing with the FeO(OH)/Fe2O3 film, which results from the disordered B2 structure Fe(Si) phase. In summary, the Fe88Si12 alloy with proper grain boundary volume fraction and composite phase structures has the best resistance in these samples.
This work was supported by the National Natural Science Foundation of China (51201172, 51275507).
- R. Wäsche and D. Klaffke, “Ceramic particulate composites in the system SiC-TiC-TiB2 sliding against SiC and Al2O3 under water,” Tribology International, vol. 32, no. 4, pp. 197–206, 1999.
- Y. S. Zhang and Z. Han, “Fretting wear behavior of nanocrystalline surface layer of pure copper under oil lubrication,” Tribology Letters, vol. 27, no. 1, pp. 53–59, 2007.
- J. Jia, Q. Ma, J. Lu, and B. Wang, “Reciprocating sliding friction and wear property of Fe3Si based alloys containing Cu in water lubrication,” Tribology Letters, vol. 30, no. 2, pp. 113–121, 2008.
- M. A. Meyers, A. Mishra, and D. J. Benson, “Mechanical properties of nanocrystalline materials,” Progress in Materials Science, vol. 51, no. 4, pp. 427–556, 2006.
- R. O. Scattergood, C. C. Koch, K. L. Murty, and D. Brenner, “Strengthening mechanisms in nanocrystalline alloys,” Materials Science and Engineering A, vol. 493, no. 1-2, pp. 3–11, 2008.
- L. Liu, Y. Li, and F. Wang, “Influence of micro-structure on corrosion behavior of a Ni-based superalloy in 3.5% NaCl,” Electrochimica Acta, vol. 52, no. 25, pp. 7193–7202, 2007.
- R. Mishra, B. Basu, and R. Balasubramaniam, “Effect of grain size on the tribological behavior of nanocrystalline nickel,” Materials Science and Engineering A, vol. 373, no. 1-2, pp. 370–373, 2004.
- Y. Lin, J. Lu, L. Wang, T. Xu, and Q. Xue, “Surface nanocrystallization by surface mechanical attrition treatment and its effect on structure and properties of plasma nitrided AISI 321 stainless steel,” Acta Materialia, vol. 54, no. 20, pp. 5599–5605, 2006.
- L. Wang, J. Ma, J. Yang, Q. Bi, L. Fu, and W. Liu, “Dry-sliding tribological properties of a nano-eutectic Fe1.87C0.13 alloy,” Wear, vol. 268, no. 7-8, pp. 991–995, 2010.
- K. R. Sriraman, S. G. Sundara Raman, and S. K. Seshadri, “Synthesis and evaluation of hardness and sliding wear resistance of electrodeposited nanocrystalline Ni-W alloys,” Materials Science and Engineering A, vol. 418, no. 1-2, pp. 303–311, 2006.
- M. Takagi, H. Ohta, T. Imura, Y. Kawamura, and A. Inoue, “Wear properties of nanocrystalline aluminum alloys and their composites,” Scripta Materialia, vol. 44, no. 8-9, pp. 2145–2148, 2001.
- D. H. Jeong, U. Erb, K. T. Aust, and G. Palumbo, “The relationship between hardness and abrasive wear resistance of electrodeposited nanocrystalline Ni-P coatings,” Scripta Materialia, vol. 48, no. 8, pp. 1067–1072, 2003.
- Z. Han, Y. Zhang, and K. Lu, “Friction and wear behaviors of nanostructured metals,” Journal of Materials Science and Technology, vol. 24, no. 4, pp. 483–494, 2008.
- L. Fu, J. Yang, Q. Bi, J. Ma, and W. Liu, “Combustion synthesis and characterization of bulk nanocrystalline Fe88Si12 alloy,” IEEE Transactions on Nanotechnology, vol. 9, no. 2, pp. 218–222, 2010.
- G. Palumbo, U. Erb, and K. T. Aust, “Triple line disclination effects on the mechanical behaviour of materials,” Scripta Metallurgica et Materiala, vol. 24, no. 12, pp. 2347–2350, 1990.
- J. F. Archard, “Contact and rubbing of flat surfaces,” Journal of Applied Physics, vol. 24, no. 8, pp. 981–988, 1953.
- C. C. Koch, I. A. Ovid'ko, S. Seal, and S. Veprek, Structural Nanocrystalline Materials: Fundamentals and Applications, Cambridge University Press, Cambridge, UK, 2007.
- Y. Toru and H. Peter, “Analysis of XPS spectra of Fe2+and Fe3+ions in oxide materials,” Applied Surface Science, vol. 254, no. 8, pp. 2441–2449, 2009.
- A. R. Lashin, O. Schneeweiss, and Y. Houbaert, “Effect of ambient air pressure on the oxidation kinetics of Fe-6 at.% Si alloy,” Corrosion Science, vol. 50, no. 9, pp. 2580–2587, 2008.
- M. D. G. M. M. Cesar and M. J. Mantel, “Effect of the temperature and dew point of the decarburization process on the oxide subscale of a 3% silicon steel,” Journal of Magnetism and Magnetic Materials, vol. 254-255, pp. 337–339, 2003.
- P. Lejček, O. Schneeweiss, and A. Fraczkiewicz, “Grain boundary segregation in an ordered Fe-24at.%Si alloy,” Surface Science, vol. 566–568, no. 1–3, pp. 826–831, 2004.
- U. Wolff, F. Schneider, K. Mummert, and L. Schultz, “Stability and electrochemical properties of passive layers on Fe-Si alloys,” Corrosion, vol. 56, no. 12, pp. 1195–1201, 2000.
- A. Atkinson, “A theoretical analysis of the oxidation of Fe-Si alloys,” Corrosion Science, vol. 22, no. 2, pp. 87–102, 1982.