micromachines Article Effects of Doping Elements on the Friction and Wear of SUJ2 Steel Sliding against Aluminum Alloys Yuh-Ping Chang *, Zi-Wei Huang and Huann-Ming Chou Department of Mechanical Engineering, Kun Shan University, Tainan 710, Taiwan; [email protected] (Z.-W.H.); [email protected] (H.-M.C.) * Correspondence: [email protected]; Tel.: +886-6-272-7175 Academic Editor: Jeng-Haur Horng Received: 7 February 2017; Accepted: 17 March 2017; Published: 23 March 2017 Abstract: Damage to mechanical components caused by wear is considered to be an important issue for mechanical engineers. For the purpose of wear resistance, it is necessary to improve the material properties of the mechanical elements. Furthermore, low friction plays an important role in saving energy. Hence, it is important to establish a key technology for wear resistance and low friction through appropriate materials science for related industries. In general, the tribological properties of aluminum alloys are very different from those of steels. Hence, aluminum alloys should be specially considered and clarified for their tribological properties before being applied industrially. This paper therefore aims to further investigate the effects of the content of doping elements on the friction and wear of the selected aluminum alloys. From the experimental results, it can be concluded that the higher the Si content, the smaller the friction coefficient, and the milder the variation. The higher the content of iron and copper, the more materials are removed, showing better machinability. Moreover, three frictional models and wear mechanisms that describe the effects of the content of doping elements on the friction and wear are proposed. The wear mechanisms change as the silicon content increases, from the junction growth to the wedge and the ploughing particles. As a result, better choices of aluminum alloys with regards to friction and wear can then be made. These results have great practical importance. Keywords: aluminum alloy; silicon; friction; wear 1. Introduction With the rapid developments of traffic vehicles and key transmission components, the demand for safe and lightweight new materials is growing, and with the global demand for energy saving and carbon reduction, the industry urgently needs to develop lightweight, reliable and environmentally friendly materials. Of the metal contained in the earth, aluminum is the second most abundant, behind iron. Hence, aluminum and its chemical compositions are the materials with large development potential [1–4]. In addition, due to its light weight, high strength, acceptable corrosion resistance and good machinability, aluminum alloy is widely used in aerospace machinery [5], defense and people’s livelihood industry. The early aluminum alloy material aimed at being lightweight, and did not consider the enhancement of wear resistance, therefore, although aluminum alloy had high strength and durability, its abrasion resistance was always significantly worse than that of steel [6]. In order to apply aluminum alloy to advanced transport vehicles and key transmission parts, further improvement of the wear properties of aluminum alloy materials is the main project of product development. Since silicon is a very strong element, if its particles are added to the industrial material, the abrasion resistance of the material can be greatly enhanced, and therefore its applicability is greatly increased [7]. Sarkar and Prasad [8,9] found that the crystal structures of silicon will affect the wear properties of aluminum alloys. If they are further mixed with an appropriate amount of Ni, Cu and Micromachines 2017, 8, 96; doi:10.3390/mi8040096 www.mdpi.com/journal/micromachines Micromachines 2017, 8, 96 2 of 12 Micromachines 2017, 8, 96 2 of 11 Mg, their mechanical properties can then be improved. Over recent decades, these research topics have been continuously investigated by national scholars [10–16]. Mg, their can then be improved. Overdegrade recent decades, these research Somemechanical researchersproperties have found that certain elements may wear properties such astopics Fe or have been continuously investigated by national scholars [10–16]. Mn. It is generally believed that this is because Fe and Mn react with silicon to produce some Some researchers havereduce foundthe thateffective certain volume elementsofmay degrade wear properties such Fe special compounds, which the silicon particles and reduce the as wear or Mn. It is generally believedrefers that this is gradual because removal Fe and Mn reactsurface with silicon to produce some properties [17]. Wear behavior to the of solid material by mechanical special which reduce the effective volumetime of the silicon particles andthe reduce the wear actions;compounds, if the wear rate is lower, a longer experimental is required to identify difference [18]. properties Wear refers to theLi gradual removal of solid surface material mechanical Moreover, [17]. Alpas, Hu,behavior and Zhang [19–21], and Tandon [22], and Subramanian [23]by designed dry actions; if the rate is lower, a longer is required toand identify theclearer difference [18]. wear tests forwear various aluminum alloys experimental to speed up time the experiments obtain results. Moreover, Alpas, Hu, andthe Zhang [19–21], Li and Tandon [22], andtemperature, Subramanianwear, [23] designed dry wear Wang [24,25] clarified relations between the frictional microstructures, tests for loads various aluminum alloys of to the speed up52100. the experiments and clearer[26–28] results. revealed Wang [24,25] normal and sliding speeds steel The studies ofobtain Moghadam that clarified the relations between the frictional temperature, wear, microstructures, normal loads the addition of suitable elements to metals decreases both the friction coefficients and wear rateand as sliding of the 52100. The Moreover, studies of Moghadam [26–28] that the addition of well as speeds increasing the steel tensile strength. the composites haverevealed good tribological properties suitable elements to metalsconditions decreases both thegraphite friction coefficients and wear well as increasing under limited lubricated due to particles acting as a rate solidaslubricant on worn the tensile strength. Moreover, the composites have good tribological properties under limited surfaces. lubricated duedocuments, to graphite particles acting as a solid lubricant on worn surfaces. Basedconditions on the above five aluminum alloys which are frequently used in industrial Based on the documents, fiveand aluminum alloys which are frequently industrial circles are used in above this study for friction wear experiments, in order to analyzeused and in compare the circles used inelements this study orderagainst to analyze and compare the effects are of doping onfor thefriction frictionand andwear wearexperiments, of SUJ2 steel in sliding the aluminum alloys effects of doping on theconditions. friction and wear of SUJ2 steel sliding against the aluminum alloys under the selectedelements experimental under the selected experimental conditions. 2. Experimental Apparatus and Procedures 2. Experimental Apparatus and Procedures Figure 1 shows a schematic diagram of the ball/disk friction tester and the measurement Figure shows acoefficient schematic diagram of the ball/disk friction tester andbythevariations measurement system. system. The1 friction is dynamically measured and exported of electrical The friction coefficient is dynamically measured and exported by variations of electrical voltage voltage through the load cell. The electronic signals are captured by a data acquisition system, and through theare loadprocessed cell. The and electronic signals captured computer. by a data acquisition and these these data analyzed by are a personal Wear loss system, is measured and data are processed and analyzed by a personal computer. Wear loss is measured and quantitatively quantitatively analyzed by a microbalance, and microscopic wear particles are qualitatively analyzed microbalance, and microscopic wear particles are qualitatively observed by the SEM. observed by by athe SEM. Figure 1. Schematic diagram of the ball/disk friction tester with the measuring system. Figure 1. Schematic diagram of the ball/disk friction tester with the measuring system. The SUJ2 steel ball is used as the Pin, and the five aluminum alloys are alternately used as the The SUJ2 steelofball is used the 6061 Pin, and aluminum alloys arecontents alternately used the Disk, in the order 1050, 5052, as 5083, and the 7075five aluminum alloys. The of the fiveas disks Disk, in the order of 1050, 5052, 5083, 6061 and 7075 aluminum alloys. The contents of the five disks are shown in Table 1. The size and geometry of the test specimens are shown in Figure 2. The sliding are shown 1. m, Thethe sizeload andisgeometry are shown in Figure The sliding distance is in setTable to 100 set to 30 of N the andtest 60 specimens N, respectively, and the sliding2.speed is 200 distance is set to 100 m, the load is set to 30 N and 60 N, respectively, and the sliding speed is 200 mm/s mm/s in this study. The response time of this measurement system is less than 1 ms and the accuracy in response timeexperiments of this measurement system is less than 1 ms and the accuracy isRoom 0.1% is this 0.1%study. of theThe full scale. The were carried out under dry friction conditions. temperature was maintained at 25 ± 2 °C, and relative humidity was maintained at 70 ± 5%. Micromachines 2017, 8, 96 3 of 11 of the full scale. The experiments were carried out under dry friction conditions. Room temperature was maintained at 25 ± 2 ◦ C, and relative humidity was maintained at 70 ± 5%. Micromachines 2017, 8, 96 3 of 12 Table 1. Determination of the content of the five disks (wt %). Micromachines 2017, 8, 96 Table 1. Determination of the content of the five disks (wt %). Aluminum Alloys Aluminum Alloys Si Si 0.09 Si 0.09 0.09 0.27 0.09 0.58 0.27 0.60 0.58 0.60 Fe Fe Cu Cu 0.01 0.01 0.02 Cu 0.02 0.09 0.01 0.09 0.26 0.02 0.26 0.16 0.09 0.16 0.26 0.16 Mn 0.01 Mn 0.05 0.01 0.59 0.05 0.06 0.59 0.07 0.06 0.07 Mn Table 1. Determination of the content of the five disks (wt %). 1050 0.09 1050 5052 Aluminum 5052 Alloys0.09 5083 0.27 1050 5083 6061 0.58 5052 6061 7075 0.60 5083 7075 6061 7075 0.23 0.23 0.26 Fe 0.26 0.38 0.23 0.38 0.62 0.26 0.62 0.20 0.38 0.20 0.62 0.20 3 of 12 Mg 0.01 0.03 0.05 2.50 Mg 0.59 4.70 0.03 0.06 1.07 2.50 0.07 1.00 4.70 Mg 0.03 2.50 4.70 1.07 1.00 1.07 1.00 Figure 2. Size and shape of the specimens. Figure 2. Size and shape of the specimens. 3. Results and Discussion Figure 2. Size and shape of the specimens. 3. Results and Discussion 3.1. Frictionand Coefficient 3. Results Discussion 3.1. FrictionThree Coefficient reproducibility experiments were conducted. The typical results are shown in Figures 3–7. 3.1. Friction Coefficient Figure 3 shows that the average friction coefficient of 1050 is 1.1. Generally, the friction coefficient Friction coefficient Friction coefficient ,f ,f Three reproducibility experiments were conducted. The typical results are shown in Figures 3–7. Three experiments were conducted. typical are shown in Figures 3–7. changes in reproducibility the range of 1.0 to 1.2, the amplitude is The large, and results the friction frequency is high. Figure Occasionally, 3Figure shows thatduring the friction offriction 1050isis 1.1. Generally, the friction 3 shows that average the frictioncoefficient coefficient 1050 1.1. Generally, the friction coefficient theaverage experimental process, theof coefficient suddenly decreases tocoefficient 0, changeswhich in themay range 1.0the toof 1.2, the is large, the friction frequency isThe high. changes in indicate theofrange 1.0between to amplitude 1.2, the interfaces amplitude isand large, and thewear friction frequency is Occasionally, high. jitter resulting from the particles. oxidation Occasionally, the particles experimental process, the friction coefficient suddenly to 0,indicate during film the experimental the friction coefficient suddenly decreases to 0,decreases which has brokenduring into process, small between the contact interfaces, and consequently there aremay some which may indicate the jitter between the interfaces resulting from the wear particles. The oxidation variations between the frictional interfaces. The vibration amplitude of the machine is larger during the jitter between the interfaces resulting from the wear particles. The oxidation film has broken into filmexperimental has broken into small particles between the contact interfaces, and consequently there are some the small particles betweenprocess. the contact interfaces, and consequently there are some variations between the variations between the frictional interfaces. The vibration amplitude of the machine is larger during frictional interfaces. The vibration amplitude of the machine is larger during the experimental process. the experimental process. 1050-30N 1.2 1050-30N 1.1 1.2 1 1.1 0.9 0.81 0.9 0.7 0.8 0.6 0.7 0.5 0.6 0.4 0.5 0.3 0.4 0.2 0.3 0.1 0.2 0 0.1 0 10 20 30 40 50 60 70 80 90 100 0 Sliding distance (m) 80 90 100 0 10 20 30 40 50 60 70 Figure 3. Typical response of the frictiondistance coefficient(m) of 1050 alloy at 30 N. Sliding Figure 3. Typical responseofofthe thefriction friction coefficient of 1050 alloyalloy at 30 at N.30 N. Figure 3. Typical response coefficient of 1050 Micromachines 2017, 8, 96 4 of 11 Micromachines 2017, 8, 96 Micromachines 2017, 8, 96 4 of 12 4 of 12 Figure 4 shows that the average friction coefficient of 5052 aluminum alloy is about 0.85. At the Figure 4 shows that the average friction coefficient of 5052 aluminum alloy is about 0.85. At the beginningFigure of the4 friction process, the friction coefficient increases from 0.15, and the maximum friction shows that theprocess, average friction coefficient of 5052 aluminum about At the beginning of the friction the friction coefficient increases fromalloy 0.15,isand the0.85. maximum coefficient appears at friction a sliding distance 80 m. coefficient The large amplitudefrom of the friction coefficient means beginning of the process, theoffriction 0.15, and the maximum friction coefficient appears at a sliding distance of 80 increases m. The large amplitude of the friction that the friction is very severe, and because of the sharp change in the friction coefficient, it matches friction coefficient appears at a sliding distance of 80 m. The large amplitude of the friction coefficient means that the friction is very severe, and because of the sharp change in the friction coefficient means that the thelarge friction is veryamplitude severe, and because of the sharp in the friction the large vibration amplitude of the machine during thethe experiment. coefficient, it matches vibration of machine during thechange experiment. coefficient, it matches the large vibration amplitude of the machine during the experiment. Friction Frictioncoefficient coefficient, f, f 5052-30N 5052-30N 1.2 1.2 1.1 1.11 1 0.9 0.9 0.8 0.8 0.7 0.7 0.6 0.6 0.5 0.5 0.4 0.4 0.3 0.3 0.2 0.2 0.1 0.10 0 0 10 20 30 40 50 60 70 80 90 100 0 10 20 30 40 50 60 70 80 90 100 Sliding distance (m) Sliding distance (m) Figure 4. Typical response of the friction coefficient of 5052 alloy at 30 N. Figure 4. Typical response coefficientofof 5052 alloy atN. 30 N. Figure 4. Typical responseof of the the friction friction coefficient 5052 alloy at 30 The average friction coefficient of 5083 is about 0.73 as shown in Figure 5. At the beginning of Friction coefficient Friction coefficient, f, f The average friction coefficient 5083increases is about about from 0.73 in in Figure 5. coefficient At of The average friction ofof5083 is 0.73as asshown shown Figure 5. the At beginning the swings beginning the friction process, thecoefficient friction coefficient 0.9 to 1.2. The friction at of the friction process, the friction coefficient increases from 0.9 to 1.2. The friction coefficient swings at the friction frictiondistance coefficient increases from 0.9 to 1.2. Theamplitude friction coefficient swings at aroundprocess, 0.7 after the the sliding of 5 m. Moreover, it shows a large and high friction around 0.7 which after the slidingthat distance of 5 m. Moreover, it shows largeparticles amplitude and high friction frequency indicate the oxidation film has broken intoasmall between thehigh contact around 0.7 after the sliding distance of 5 m. Moreover, it shows a large amplitude and friction frequency which indicatethe that the oxidation film has broken into small particles between the contact interfaces. Asindicate a result, amplitude of the machine larger during the experimental frequency which that vibration the oxidation film has broken intoissmall particles between the contact interfaces. As a result, the vibration amplitude of the machine is larger during the experimental process. interfaces. As a result, the vibration amplitude of the machine is larger during the experimental process. process. 5083-30N 1.2 5083-30N 1.2 1.1 1.11 1 0.9 0.9 0.8 0.8 0.7 0.7 0.6 0.6 0.5 0.5 0.4 0.4 0.3 0.3 0.2 0.2 0.1 0.10 0 0 10 20 30 40 50 60 70 80 90 100 0 10 20 30 40 50 60 70 80 90 100 Sliding distance (m) Sliding distance (m) Figure 5. Typical response of the friction coefficient of 5083 alloy at 30 N. Figure 5. Typical response coefficientofof 5083 alloy atN. 30 N. Figure 5. Typical responseof of the the friction friction coefficient 5083 alloy at 30 Micromachines 2017, 8, 96 5 of 11 Micromachines 2017, 8, 96 5 of 12 The friction coefficient shown in Figure 6 is between that in Figures 4 and 5; it is representative of a few exceptions in the series. It shows that the average friction coefficient of 6061 aluminum alloy is The friction coefficient shown in Figure 6 is between that in Figures 4 and 5; it is representative about 0.9, and the friction high. coefficient During the Micromachines 2017, 8, 96 is 5 of 12process, of athe fewamplitude exceptions in large the series. It shows thatfrequency the averageisfriction of experimental 6061 aluminum the friction changesisvery Thisfrequency may indicate the jitter the between the interfaces alloycoefficient is about 0.9,value the amplitude largedrastically. and the friction is high. During experimental Thethe friction coefficient shown in changes Figurethe 6 very istemperature between that in Figures 4indicate andthe 5; itfriction is representative process, the friction coefficient value drastically. This may the jitter process between [24,25], resulting from wear particles. Moreover, rises during of a few exceptions in the series. It shows that the average friction coefficient of 6061 the aluminum the interfaces resulting from the wear particles. Moreover, the temperature rises during and the material is therefore softened, resulting in adhesion; and the softened surfacefriction is ploughed, alloy is about 0.9,and the the amplitude is large and thesoftened, friction frequency Duringand the experimental process [24,25], material is therefore resulting isinhigh. adhesion; the softened generating a large and long slip tongue. process, the friction coefficient value changes very drastically. This may indicate the jitter between surface is ploughed, generating a large and long slip tongue. the interfaces resulting from the wear particles. Moreover, the temperature rises during the friction process [24,25], and the material is therefore softened, resulting in adhesion; and the softened 6061-30N surface is ploughed, generating 1.2 a large and long slip tongue. coefficient ,f FrictionFriction coefficient ,f 1.1 1 6061-30N 1.2 0.9 1.1 0.8 0.71 0.9 0.6 0.8 0.5 0.7 0.4 0.6 0.3 0.5 0.2 0.4 0.1 0.3 0 0.2 0 10 20 30 40 50 60 70 80 90 100 0.1 Sliding distance (m) 0 0 10 20 30 40 50 60 70of 6061 80 alloy 90 at 100 Figure 6. Typical response of the friction coefficient 30 N. Figure 6. Typical response of the friction coefficient of 6061 alloy at 30 N. Sliding distance (m) The average friction coefficient of 7075 aluminum alloy is about 0.7 as shown in Figure 7. At Figure 6. Typical response of thealuminum friction coefficient of 6061 alloy0.5, at 0.7 30 N.as the beginning of the friction process, friction coefficient increases and theshown maximum The average friction coefficient ofthe7075 alloy is from about in of Figure 7. friction coefficient appears at a sliding distance of 38 m. This may indicate that the temperature At the beginning of the friction process, the friction coefficient increases from 0.5, and the maximum of average frictionprocess, coefficient 7075 aluminum alloy is about 0.7 as shown in Figure At rises The during the friction the of material is therefore softened, resulting in adhesion, and7.low friction frequency coefficient appears atand a sliding distance ofcoefficient 38is m. This may indicate the temperature rises the beginning of arises; the friction process, the friction increases from 0.5,a that and the maximum of wear the softened surface ploughed, generating large and long slip during the friction process, the material is therefore softened, resulting in adhesion, and low frequency friction coefficient appears at a sliding distance of 38 m. This may indicate that the temperature tongue. As a result, the response frequency of the friction coefficient is low. On the other hand, the rises during friction the material is therefore softened, in adhesion, and As lowa result, wear arises; and thethesoftened surface iswith ploughed, generating a large and long slip friction coefficient slightlyprocess, increases the sliding distance until theresulting experiment ends.tongue. frequency wear arises; and the softened surface is ploughed, generating a large and long the response frequency of the friction coefficient is low. On the other hand, the friction slip coefficient tongue. As a result, the response7075-30N frequency of the friction coefficient is low. On the other hand, the slightly increases with the sliding distance until the experiment ends. friction coefficient slightly1.2 increases with the sliding distance until the experiment ends. coefficient ,f Friction Friction coefficient ,f 1.1 1 7075-30N 1.2 0.9 1.1 0.8 0.71 0.9 0.6 0.8 0.5 0.7 0.4 0.6 0.3 0.5 0.2 0.4 0.1 0.3 0 0.2 0 10 20 30 40 50 60 70 80 90 100 0.1 Sliding distance (m) 0 0 response 10 20of 30 40 50coefficient 60 70of 7075 80 alloy 90 100 Figure 7. Typical the friction at 30 N. Sliding distance (m) Figure 7. Typical response of the friction coefficient of 7075 alloy at 30 N. Figure 7. Typical response of the friction coefficient of 7075 alloy at 30 N. Micromachines 2017, 8, 96 6 of 11 According to the above results of the friction coefficient and the data in Table 1, it is shown that as the Si content gradually increases, the friction coefficient of the material with a higher percentage of Si decreases. Micromachines 2017, 8, 96 3.2. Wear Loss 6 of 12 According to the above results of the friction coefficient and the data in Table 1, it is shown as the Si contentexperiments gradually increases, friction coefficient of the of material with a higher Threethat reproducibility were the conducted. The results the average wear loss are percentage of Si decreases. shown in Figure 8. As shown in Figure 8a of 30 N, the average wear loss of 1050 aluminum alloy is 37 mg;3.2. 51Wear mgLoss for 5052 aluminum alloy; 38 mg for 5083 aluminum alloy; 60 mg for 6061 aluminum alloy; and 38 mg for 7075 aluminum alloy. In Figure 8b of 60 N, the average wear loss of Three reproducibility experiments were conducted. The results of the average wear loss are 1050 aluminum 78inmg for8a5052 aluminum 57ofmg 5083 aluminum alloy; shown inalloy Figureis8.44 As mg, shown Figure of 30 N, the averagealloy; wear loss 1050for aluminum alloy is 153 mg for376061 aluminum alloy; and 58 mg38for aluminum Hence, wear losses mg; 51 mg for 5052 aluminum alloy; mg7075 for 5083 aluminumalloy. alloy; 60 mg forthe 6061average aluminum alloy; andto38the mg normal for 7075 aluminum alloy.indicates In Figure that 8b of the 60 N,wear the average of 1050Moreover, are proportional loads. This modeswear are loss regular. aluminum alloy is 44 mg, 78 mg for 5052 aluminum alloy; 57 mg for 5083 aluminum alloy; 153 mg the average wear loss of 6061 aluminum alloy is especially larger. Compared to the data in Table 1, for 6061 aluminum alloy; and 58 mg for 7075 aluminum alloy. Hence, the average wear losses are the higherproportional the contents of iron and copper, the more materials are removed, representing better to the normal loads. This indicates that the wear modes are regular. Moreover, the machinability. Since Cu/Fe pairs are compatible, this indicates that the wear average wearthe lossFe/Fe of 6061 and aluminum alloy is especially larger. Compared to the data in Table 1, the losses for higher doping the contents of ironare andlarger copper,[18]. the On morethe materials are removed, representing the compatible elements other hand, it is worth notingbetter that the wear machinability. Since the Fe/Fe and Cu/Fe pairs are compatible, this indicates that the wear losses loss of 5083 is quite small. This indicates that a higher content of Mn or Mg is harmlessfor to the wear the compatible doping elements are larger [18]. On the other hand, it is worth noting that the wear loss. Namely, if the pairs are incompatible, the wear losses are smaller [18]. As aluminum alloys are loss of 5083 is quite small. This indicates that a higher content of Mn or Mg is harmless to the wear relatively soft and have a lower melting point, the wear particles produced in the friction process easily loss. Namely, if the pairs are incompatible, the wear losses are smaller [18]. As aluminum alloys are relatively soft andinterfaces, have a lowerand melting the wear particles in the heat friction processin material deviate from the contact the point, high temperature dueproduced to frictional results easily deviate from the contact interfaces, the track high temperature to frictionalofheat transfer. Therefore, optical microscopy of theand wear and SEM due observation theresults wearinparticle are material transfer. Therefore, optical microscopy of the wear track and SEM observation of the wear both required for observing the wear mechanisms. particle are both required for observing the wear mechanisms. Figure 8. Average wear loss of the five alloys: (a) 30 N; (b) 60 N. Figure 8. Average wear loss of the five alloys: (a) 30 N; (b) 60 N. 3.3. Optical Microscopy of the Wear Track Figure 9 shows that the wear surface of the 1050 aluminum alloy presents rough wavy scratching at different widths, meaning that the vibration is relatively violent for the SUJ2 ball sliding against Micromachines 2017, 8, 96 7 of 11 this material, i.e., there is significant material transfer and deformation during the friction process. 2017, 8, x FOR PEER REVIEW and adhere to areas outside the wear marks. This 8 of can 13 As a result,Micromachines many materials are extruded be used to demonstrate that while the material is soft, the wear loss is not the largest. X100 (a) 30 N (b) 60 N 1050 5052 5083 6061 7075 Figure 9. Optical microscopy of the wear track of the five alloys: (a) 30 N; (b) 60 N. Figure 9. Optical microscopy of the wear track of the five alloys: (a) 30 N; (b) 60 N. The wear scratching of 5052 aluminum alloy is similar to the case of 1050 aluminum alloy, the surfaces of which present rough and wavy scratching in different widths, the vibration is slightly violent and there is some material transfer and deformation during the friction process. Thus, part of the materials that are extruded adhere to areas outside the wear marks. Moreover, it is believed that high temperatures result in material transfer and deformation during the friction process of 1050 and 5052 aluminum alloys, and the friction scratching presents many crash and melting patterns. Micromachines 2017, 8, 96 8 of 11 For 5083 aluminum alloy, the friction marks are narrower but deeper than for 1050 or 5083 aluminum alloys. This means that the wear mechanism of 5083 aluminum alloy is quite different from that of 1050 or 5083 aluminum alloys. The wear surface of 6061 aluminum alloy is wide but with smooth friction tracks. Since the 7075 alloy sample has the highest hardness, it is to be expected that the scratched wear surface is the smoothest and the friction tracks are the narrowest. Moreover, the scratched wear surfaces of 6061 and 7075 aluminum alloys look quite smooth. These results match the previous results of wear loss. 3.4. SEM Observation of Wear Particle Figure 10 shows that the wear particles of 1050 and 5052 aluminum alloys are flake-like and laminated; it can be reasonable explained by the fact that these materials are relatively soft and have a lower melting point, thus resulting in deformation and material transfer due to high temperature during the friction process. A large number of wear particles of large size can be found. The large wear particles are caused by the junction growth during the adhesive wear. Therefore, in these experiments, the friction coefficient is larger than the other cases due to the action of the junction growth [29]. Micromachines 2017, 8, x FOR PEER REVIEW 30N X35 10 of 13 X100 X500 1050 5052 5083 6061 7075 Figure 10. SEM of wear particle of the five alloys. Figure 10. SEM of wear particle of the five alloys. 3.5. Frictional Models and Wear Mechanisms By considering all of the above aluminum experimental alloy results materials as well as the by the Most of the wear particles of 5083 areprevious similarstudies to those of 1050 and authors [29–31], three frictional models and wear mechanisms that describe the effects of the content 5052 aluminum alloy materials. Moreover, it is worth noting that some thick ridge-like particles are of doping elements on the friction and wear of SUJ2 steel sliding against aluminum alloys are proposed. It is observed from Figure 11a that the flake-like particles resulted from the higher adhesion at the junction growth region for the low content of silicon (only 0.09%): 1050 and 5052 aluminum alloys. Hence, more friction is caused. Figure 11b shows that medium adhesion is present at the interfaces for the medium content of silicon (0.27%): 5083 aluminum alloy. The flake-like particles with some wedge particles were developed from both the junction growth and the adhesive transfer of the wedge. Figure 11c shows that the relatively large ploughing particles were caused by Micromachines 2017, 8, 96 9 of 11 observed and the fracture mechanism of the wedge can be revealed. The wedge growth by plowing is quite significant. It is believed that the thick ridge-like particles result from the adhesive transfer of the wedge [30]. The 6061 and 7075 aluminum alloy materials produce strip-shaped wear particles. Several examples of ploughed particles are shown. In these two cases, ploughing is comparatively significant and large. It is believed that the ploughing wear particles are caused by grooving wear during the wear test [31]. 3.5. Frictional Models and Wear Mechanisms By considering all of the above experimental results as well as the previous studies by the authors [29–31], three frictional models and wear mechanisms that describe the effects of the content of doping elements on the friction and wear of SUJ2 steel sliding against aluminum alloys are proposed. It is observed from Figure 11a that the flake-like particles resulted from the higher adhesion at the junction growth region for the low content of silicon (only 0.09%): 1050 and 5052 aluminum alloys. Hence, more friction is caused. Figure 11b shows that medium adhesion is present at the interfaces for the medium content of silicon (0.27%): 5083 aluminum alloy. The flake-like particles with some wedge particles were developed from both the junction growth and the adhesive transfer of the wedge. Figure 11c shows that the relatively large ploughing particles were caused by the grooving wear mechanism for the high content of silicon (~0.6%): 6061 and 7075 aluminum alloys. Hence, less friction is caused due to the lower Micromachines 2017, 8, 96 adhesion. These results correspond to the previous friction 10 of 12 coefficient responses. Wear mechanisms change as the silicon content increases, from the junction growth to the previous friction coefficient responses. Wear mechanisms change as the silicon content increases, wedge particles, and even to the ploughing particles. from the junction growth to the wedge particles, and even to the ploughing particles. Figure 11. Frictional models and wear mechanisms of SUJ2 steel sliding against Al–Si alloys: (a) Low Figure 11. Frictional models and wear mechanisms of SUJ2 steel sliding against Al–Si alloys: (a) Low content of silicon: 1050 and 5052 aluminum alloys; (b) Medium content of silicon: 5083 aluminum content of silicon: and 5052 aluminum alloys; (b) Medium content of silicon: 5083 aluminum alloy; (c)1050 High content of silicon: 6061 and 7075 aluminum alloys. alloy; (c) High content of silicon: 6061 and 7075 aluminum alloys. 4. Conclusions From the variations of the friction coefficient with optical microscopy and SEM observations of the wear, the following conclusions have been drawn: 1. The materials with a higher Si content percentage show lower friction. Generally, the friction coefficient decreases with increases in the Si content, and the variation of the friction coefficient is milder. Micromachines 2017, 8, 96 10 of 11 4. Conclusions From the variations of the friction coefficient with optical microscopy and SEM observations of the wear, the following conclusions have been drawn: 1. 2. 3. 4. The materials with a higher Si content percentage show lower friction. Generally, the friction coefficient decreases with increases in the Si content, and the variation of the friction coefficient is milder. The 6061 aluminum alloy has severe ploughing and wear particles. The wear losses for the compatible doping elements are larger. Therefore, the higher the contents of iron and copper, the more materials are removed, representing better machinability. Three frictional models and wear mechanisms that describe the effects of the content of doping elements on the friction and wear of SUJ2 steel sliding against aluminum alloys are proposed. The wear mechanisms change as the silicon content increases, from the junction growth to the wedge and the ploughing particles. Based on the above three models, better choices of aluminum alloys with regards to friction and wear can be made. These results have great practical importance for the precision machinery industry. Acknowledgments: The authors would like to express their appreciation to the National Science Council in Taiwan for their financial support under grant number MOST 105-2622-E-150-001-CC2 and MOST 105-2221-E-168-004. Author Contributions: Yuh-Ping Chang, Zi-Wei Huang and Huann-Ming Chou conceived and designed the experiments; Zi-Wei Huang performed the experiments; Yuh-Ping Chang, Zi-Wei Huang and Huann-Ming Chou analyzed the data; Yuh-Ping Chang and Zi-Wei Huang wrote the paper; Yuh-Ping Chang revised the paper. All authors read and approved the final manuscript. Conflicts of Interest: The authors declare no conflict of interest. References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. Du, J.; Wei, Z.; Chen, Z.; Li, S.; Tang, Y. Numerical investigation of pileup process in metal microdroplet deposition manufacture. Micromachines 2014, 5, 1429–1444. [CrossRef] Florian, P.; Benedikt, A.; Ralf, H. Micromachining of AlN and Al2 O3 using fiber laser. Micromachines 2014, 5, 1051–1060. Yang, J.; Si, C.; Han, G.; Zhang, M.; Ma, L.; Zhao, Y.; Ning, J. Researching the aluminum nitride etching process for application in MEMS resonators. Micromachines 2015, 6, 281–290. [CrossRef] Zhang, M.; Yang, J.; Si, C.; Han, G.; Zhao, Y.; Ning, J. Research on the piezoelectric properties of AlN thin films for MEMS applications. Micromachines 2015, 6, 1236–1248. [CrossRef] Lane, J. Aluminium in Building; Ashgate Publish Ltd.: Hants, UK, 1992. Krishna Kanth, V.; Pramila Bai, B.N.; Biswas, S.K. Wear mechanisms in a hypereutectic aluminum silicon alloy sliding against steel. Scr. Metall. Mater. 1990, 24, 267–271. [CrossRef] Torabian, H.; Pathak, J.P.; Tiwari, S.N. Wear characteristics of Al-Si alloys. Wear 1994, 172, 49–58. [CrossRef] Sarkar, A.D. Wear of aluminium-silcon. Wear 1975, 31, 331–343. Prasad, B.K.; Venkateswarlu, K.; Modi, O.P.; Jha, A.K.; Das, S.; Dasgupta, R.; Yegneswaran, A.H. Sliding wear behavior of some Al-Si alloys: Role of shape and size of Si particles and test conditions. Metall. Mater. Trans. A 1998, 29, 2747–2752. [CrossRef] Smith, W.F. Structure and Properties of Engineering Alloys, 2nd ed.; McGraw-Hill: New York, NY, USA, 1993. Saeid, F.; Saeid, M. Effect of material structure machining characteristics of hypereutectic Al-Si alloy. Mech. Adv. Manuf. Technol. 2007, 4–15. Birol, Y. Cooling slope casting and thixoforming of hypereutectic A390 alloy. J. Mater. Process. Technol. 2008, 207, 200–203. [CrossRef] Rios, P.R.; Fonseca, G.S. Grain boundary pinning by Al6Mn precipitates in an Al-1wt % Mn alloy. Scr. Mater. 2004, 50, 71–75. [CrossRef] Reddy, A.S.; Bai, B.N.P.; Murthy, K.S.S.; Biswas, S.K. Wear and seizure of binary Al-Si alloys. Wear 1994, 171, 115–127. [CrossRef] Micromachines 2017, 8, 96 15. 16. 17. 18. 19. 20. 21. 22. 23. 24. 25. 26. 27. 28. 29. 30. 31. 11 of 11 Reddy, A.S.; Bai, B.N.P.; Murthy, K.S.S.; Biswas, S.K. Mechanism of seizure of aluminium-silicon alloys dry sliding against Steel. Wear 1995, 181–183, 658–667. [CrossRef] Wert, J.A. Microstructures of friction stir weld joints between an aluminum-base metal matrix composite and a monolithic aluminum alloy. Scr. Mater. 2003, 49, 607–612. [CrossRef] Yamauch, S.; Shibue, K.; Okubo, Y.; Sano, H.; Inumalu, S. Development of wear-resistant P/M aluminum alloys “PA4XX”. Bull. Jpn. Inst. Met. 1988, 27, 492–494. [CrossRef] Rabinowicz, E. Friction and Wear of Materials, 2nd ed.; Wiley-Interscience: New York, NY, USA, 1995; pp. 38–39, 84–88. Alpas, A.T.; Zhang, J. Wear rate transitions in cast aluminum-silicon alloys reinforced with SiC particles. Scr. Metall. Mater. 1992, 26, 505–509. Zhang, J.; Alpas, A.T. Delamination wear in ductile materials containing second phase particles. Mater. Sci. Eng. A 1993, 160, 25–35. [CrossRef] Alpas, A.T.; Hu, H.; Zhang, J. Plastic deformation and damage accumulation below the worn surfaces. Wear 1993, 162–164, 188–195. [CrossRef] Li, X.Y.; Tandon, K.N. Mechanical mixing induced by sliding wear of an Al-Si alloy against M2 steel. Wear 1999, 225–229, 640–648. Subramanian, C. On mechanical mixing during dry sliding of aluminium-12.3 wt % silicon alloy against copper. Wear 1993, 161, 53–60. Wang, Y.; Li, X.D.; Feng, Z.C. The relationship between the product of load and sliding speed with friction temperature and sliding wear of a 52100 steel. Scr. Metall. Mater. 1995, 33, 1163–1168. [CrossRef] Wang, Y.; Yan, M.; Li, X.D.; Lei, T. Frictional temperature field and wear behavior of steel 52100 with different microstructures. J. Tribol. 1994, 116, 255–259. [CrossRef] Moghadam, A.D.; Omrani, E.; Menezes, P.L.; Rohatgi, P.K. Mechanical and tribological properties of self-lubricating metal matrix nanocomposites reinforced by carbon nanotubes (CNTs) and grapheme—A review. Compos. Part B Eng. 2015, 77, 402–420. [CrossRef] Moghadam, A.D.; Schultz, B.F.; Ferguson, J.B.; Omrani, E.; Rohatgi, P.K.; Gupta, N. Functional metal matrix composites: Self-lubricating, self-healing, and nanocomposites—An Outlook. JOM 2014, 66, 872–881. [CrossRef] Omrani, E.; Moghadam, A.D.; Algazzar, M.; Menezes, P.L.; Rohatgi, P.K. Effect of graphite particles on improving tribological properties Al-16Si-5Ni-5Graphite self-lubricating composite under fully flooded and starved lubrication conditions for transportation applications. Int. J. Adv. Manuf. Technol. 2016, 87, 929–939. [CrossRef] Chiou, Y.C.; Chang, Y.P.; Lee, R.T. Tribo-electrification mechanism for self-mated metals in dry severe wear process, part II: Pure soft metals. Wear 2003, 254, 616–624. [CrossRef] Chang, Y.P.; Yur, J.P.; Chou, H.M.; Chu, H.M. Tribo-electrification mechanisms for self-mated carbon steels in dry severe wear process. Wear 2006, 260, 1209–1216. [CrossRef] Chang, Y.P.; Chu, H.M.; Chou, H.M. Effects of mechanical properties on the tribo-electrification mechanisms of iron rubbing with carbon steels. Wear 2007, 262, 112–120. [CrossRef] © 2017 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).
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