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Article

Effects of Reinforcement Volume Fraction on Mechanical Properties and Microstructures of 7075Al Matrix Composites Reinforced by FeCoCrNiAl High-Entropy Alloy Particles

State Key Laboratory of Advanced Processing and Recycling of Nonferrous Metals, School of Materials Science and Engineering, Lanzhou University of Technology, Lanzhou 730050, China
*
Authors to whom correspondence should be addressed.
Metals 2022, 12(5), 851; https://doi.org/10.3390/met12050851
Submission received: 13 April 2022 / Revised: 12 May 2022 / Accepted: 13 May 2022 / Published: 16 May 2022

Abstract

:
High-entropy alloy particles reinforcements improve the mechanical properties of aluminum matrix composites while increasing its density. Investigating the effects of the reinforcement content is conducive to the fabrication of lightweight and high strength composites. FeCoCrNiAl high-entropy alloy particles (HEAp) reinforced 7075Al matrix composites (HEAp/Al) with different HEAp volume fractions of 5, 10, 15, and 20 vol% were fabricated via a vacuum ball milling and vacuum hot pressing sintering, and then the microstructures, interface, density, and mechanical properties of the HEAp/Al composites were characterized. The results indicated that composites with high relative density can be obtained with a holding time of 10 min at 580 °C, 30 MPa; the HEAp distribution was homogeneous as the increase of reinforcement volume fraction decreases and forms agglomeration, especially when the volume fraction is up to 15 vol% and 20 vol%; the density and hardness of HEAp/Al composites improved with the increase of reinforcements’ volume fraction, whereas the flexural strength and fracture toughness of HEAp/Al composites increased at first and then decreased; the HEAp/Al composites reinforced by 10 vol% HEAp showed the maximum flexural strength and fracture toughness, which were increased by 124.6% and 107% compared with 7075Al, respectively; the improvement of mechanical properties was attributed to the dislocation strengthening behavior and load transfer effect of the HEAp reinforcement.

1. Introduction

Owing to their excellent characteristics, such as low density, high specific strength and modulus, good dimensional stability, and wear resistance, aluminium matrix composites have a wide application prospect in aerospace engineering, military area, and automotive fields [1,2]. According to the reinforcement types, Al matrix composites can be divided into two kinds, such as discontinuous reinforcement reinforced Al matrix composites and continuous reinforcement reinforced Al matrix composites. Interestingly, Al matrix composites reinforced by discontinuous reinforcement, having better machinability and isotropic properties compared with continuous fiber reinforced aluminum matrix composites, is one kind of the most widely used composites in engineering practice. The traditional discontinuous reinforcements, including Al2O3 [3], SiC [4], BN [5] and other ceramic particles, have obvious thermal expansion mismatch with Al matrix, which can lead to the generation of microcracks and defects in composites and weaken the strengthening effect of reinforcements. As one rare species of metal materials, high-entropy alloys have excellent corrosion properties and physical properties [6,7,8,9], including high strength, high hardness, high modulus, and high thermal stability, and can form a good metallurgical bonding interface with Al [10]; these characteristics illustrate that high-entropy alloys can meet the performance requirements of ideal reinforcements used for Al matrix composites.
Currently, research on high-entropy alloys reinforced Al matrix composites have been reported. Zhu et al. [11] studied the effect of the particle shapes of Al0.23Cu0.75FeCoNi high-entropy alloy reinforcements on the properties of Al matrix composites and found that flake particles were easy to agglomerate in the matrix, which would cause the initiation of microvoids so that the failure mode of composites was dominated by the rupture of agglomeration. Conversely, ellipsoidal particles were not only beneficial to the uniform distribution of reinforcements, but also effectively inhibited stress concentration between reinforcement and matrix—Yuan et al. [12] studied the interface microstructure on mechanical properties of 5052Al matrix composites reinforced with 7 vol% content of Al0.6CoCrFeNi, and found that core-shell structure forming at interface without new phase generated between reinforcements and matrix improved Young’s modulus and hardness of Al matrix composites. The compressive properties of FeNiCrCoAl3 reinforced 2024Al composites fabricated by two-stage method consisting of ball milling and hot extrusion were studied in ref. [13], in which composites showed excellent compressive strength with the values of 700 MPa compared with the 2024Al matrix. Karthik et al. [14] realized that the tensile and compressive properties of AA5083 matrix composites can be improved by the addition of CoCrFeNi nanocrystalline high-entropy alloy particles, and the composites possessed much better combination of strength and ductility compared with conventional Al matrix composites reinforced by ceramic particles. Also, the high-entropy alloy could improve the wear resistance, and macro- and micro-hardness [15,16] of metal matrix composites. Especially, thermal expansion coefficient of high-entropy alloy particle reinforced Al matrix composites decreased as high-entropy alloy volume fraction increased [17], and even could be compared favourably with those of ceramic particles reinforced Al matrix composites [18,19]. Nevertheless, the addition of high-entropy alloy particles with high density (>6 g/cm3) would weaken the lightweight advantages of Al matrix composites with the improving of mechanical properties. Controlling the content of high-entropy alloy reinforcement in composites is significant for the fabrication of lightweight composites on the premise of maximally optimizing the properties of the alloy matrix. Unfortunately, there were few reports about the effect of reinforcement on the combination of density and mechanical properties.
With a high microhardness [20], specific strength, Young’s modulus [21], certain ductility [22], and excellent thermal stability [23], FeCoCrNiAl high-entropy alloy particles (HEAp) with face-centered cubic structure, can be obtained using powder metallurgy method with low energy consumption [24], and used in Al matrix composites as metal particle reinforcement with ideal performance. In this work, 7075Al powders and FeCoCrNiAl high-entropy alloy particles powders were used for the matrix and reinforcement, respectively. FeCoCrNiAl HEAp reinforced 7075Al composites (HEAp/Al) with different volume fractions of reinforcement were prepared by vacuum ball milling firstly and then a hot pressing sintering process. By characterization of microstructure, density, and mechanical properties of composites, the effects of volume fraction of reinforcements on mechanical performances of HEAp/Al were revealed so that a theoretical reference could be provided for the fabrication of lightweight high performances aluminum matrix composites.

2. Experimental

2.1. Fabrication of HEAp/Al Composites

FeCoCrNiAl high-entropy alloy particle reinforcements (HEAp) were provided by Beijing Gaoke New Materials Co., Ltd., Beijing, China, and particles with size of about 13 μm are regular spherical. 7075Al spherical powders (provided by Hebei Qinbang New Material Co., Ltd., Shijiazhuang, China) with particle diameter of about 25 μm were used for aluminum matrix.
The fabrication process of FeCoCrNiAl HEA particles reinforced 7075Al composites (HEAp/Al) is illustrated in Figure 1; its procedure proceeded as follows: Firstly, the mass of HEAp was calculated on the scales of 5, 10, 15, and 20 vol% of composites respectively, and then weighed using an electronic analytical balance (AUW120D, Shimadzu Co., Tokyo, Japan) to obtain the scheduled mass, while the scheduled mass of 7075Al powder was weighed in a similar way with the volume fraction of 95, 90, 85 and 80 vol% respectively; secondly, the scheduled HEAp and 7075Al were put into sealed ball milling jars, and then the jars were filled with high purity Ar with 0.04 MPa for oxidation protection. The mixing powders were milled for 6 h with a milling rate of 300 r/min under a certain ball to powders weight ratio of 10:1; lastly, the milled powders were packed into graphite mold, and successively vacuum sintered using program control vacuum sintering instrument (RYJ-2000Z, Zhengzhou abrasive grinding Research Institute Co., Zhengzhou, China) at 580 °C, 30 MPa for 10 min. In order to reduce cavity defects in composites, the heating temperature was held for 5 min at 420 °C. After cooling with furnace, the HEAp/Al composites with different HEAp volumes were prepared.

2.2. Testing and Characterization

According to the YB/T 5349-2014 and ASTM E1304-97 (2020) standards, three-point bending samples with 3 mm × 4 mm × 30 mm long stripe and fracture toughness test samples with the size of 3 mm × 4 mm × 30 mm (integral notch, depth 2 mm) were processed by the cutting of HEAp/Al composites using wire electro-discharge machining, and successively polished the surface of the samples through 240, 400, 600, 800, 1000, 1500# metallographic water-resistant sandpaper. The tests on flexural strength and fracture toughness of HEAp/Al composites were carried out on an electronic universal testing machine (MTS E44.304, MTS Systems Co., Eden Prairie, MN, USA) with a constant movement rate of 0.3 and 0.1 mm/min respectively at ambient temperature. Each final value represents the average result of three measurements to ensure the accuracy and repetitiveness of measured results.
The phase components of HEAp/Al composites were characterized from 20° to 80° with a scanning rate of 6°/min using x-ray diffractometer (D8 ADVANCE, Bruker AXS Co., Karlsruhe, Germany). The densities of HEAp/Al composites with different reinforcement contents were tested using the automatic density measuring instrument (MH-300A, Xiamen east equipment Co., Ltd., Xiamen, China). Rockwell hardness of HEAp/Al composites was characterized using an electric Rockwell hardness tester (HRD-150, Lailuote experiment instrument Co., Ltd., Yantai, China), the average value of seven points was selected as final value. Lastly, the microstructures, interface element distribution, and fracture morphologies were investigated using a scanning electron microscope with an energy spectrometer (JSM-6510SEM, JEOL Ltd., Tokyo, Japan) and transmission electron microscope (FEI Talos F200X TEM, FEI Co., Hillsboro, OR, USA).

3. Results and Discussion

3.1. X-ray Diffraction Patterns of HEAp/Al Composites

The X-ray diffraction patterns of unreinforced 7075Al and HEAp/Al composites with 10 vol% HEAp content are shown in Figure 2. Visibly, crystal diffraction peaks with high diffraction intensity of Al occur at 38.5° (2θ), 44.7° (2θ), 65.1° (2θ), and 78.2° (2θ), which were corresponding to (111), (200), (220) and (311) crystal planes respectively. In addition, the phase diffraction peaks of Al12Mg17, AlCuMg, and AlZn Al0.403Zn0.597 with weak diffraction intensity present in the spectrum, indicate that the elements Mg, Cu, and Zn reacted with Al to form intermetallic compounds. After the addition of HEAp, the crystal diffraction peaks of HEAp and Al9Co2 occur at the HEAp/Al patterns with the exception of Al and its compounds. Notably, Al0.403Zn0.597 (PDF# 52-0856) and Al diffraction angles (PDF#89-4037) were similar; they were represented by the same symbol. These results prove that the HEAp still maintained a complete structure, while the metallurgical bonding was formed at the interface between reinforcements and matrix.

3.2. Microstructure of HEAp/Al Composites

Figure 3 shows microstructure morphologies of HEAp/Al composites reinforced with 5, 10, 15 and 20 vol% HEAp respectively. As shown in Figure 3a,b, HEAp reinforcements are distributed homogeneously in the matrix when the HEAp volume fraction did not exceed 10 vol%. However, the distribution uniformity of HEAp become worse as the HEAp content was up to 15 vol% and 20 vol% respectively, and there are a small amount of particle agglomeration occurring in the 7075Al matrix (shown in Figure 3c,d). Besides, the accompanying diagram of Figure 3b illustrates that element line scanning obviously varies from Al matrix to HEAp, which indicates that HEAp still maintained the original regular spherical without obvious melting and crushing, which was corresponding to the presence of HEAp diffraction apex in X-ray diffraction analysis of HEAp/Al composites.
The distribution uniformity of reinforcements in the matrix plays an important role in the properties of composites, and is mainly affected by the volume fraction and particle diameter of reinforcements and matrix. The critical volume fraction Wcrit of reinforcements with a homogeneous distribution is calculated by the formula of Equation (1) shown as follows [17]:
W crit = α × V r V r + V m = α × { 1 [ 1 + ( d D ) 3 + ( 2 λ + λ ) × ( d D ) 2 + ( 1 λ + 2 λ ) × d D ] 1 }
where α represents the fixed parameter with the value of 0.18, d and D refers to the particle size medium diameter of HEAp (d = −13 μm) and 705Al matrix (D = −25 μm) respectively, and λ indicates the extrusion ratio (the value of λ without extrusion is 1). The values of Wcrit of HEAp calculated using Equation (1) is about 12.87 vol%, which means particle agglomeration became serious in the matrix when the reinforcement content exceeded 12.87 vol%. Thus, the particle agglomeration of HEAp/Al composites with 20 vol% HEAp is more serious than that of HEAp/Al composites with 15 vol% HEAp.

3.3. Interface Microstructure of HEAp/Al Composites

The energy-dispersive X-ray spectroscopy (EDS) mappings of elements Al, Co, Cr, Ni, Fe and Mg at the interface between HEAp and 7075Al matrix are shown in Figure 4. Clearly, there is an obvious boundary formed at the interface caused by the heterogeneity of elemental distribution, which was similar to the line distribution of elements. Notably, the element Mg is accumulated around the HEAp, which was caused by the difference of bonding energy between elements. The enthalpy of mixing (∆Hmix) between elements Al and Mg is −2 Kj/mol; its absolute value is lower than that of Mg-Ni (−4 Kj/mol) [25], and there is an interdiffusion formed between Ni and Mg. However, the interdiffusion between Mg and Ni is suppressed by the high stability of HEAp so that the Mg elements enrichment area was formed at the interface between HEAp and 7075Al matrix.
Interface microstructure between HEAp and 7075Al matrix is shown in Figure 5. As shown in Figure 5a,b, an obvious boundary with incoherent lattice is formed between HEAp and 7075Al. Besides, many dislocations can be found around the HEAp in the 7075Al matrix, which are generated and stored because of thermal expansion coefficient mismatch.
The density parameters reveal indirectly the defect content of composites and evaluate effectively the reasonability of the sintering process. The measured density and relative density of HEAp/Al composites with various HEAp volume fractions are shown in Figure 6. Clearly, the measured density of HEAp/Al composites increase as the HEAp volume fraction improved from 0 vol% to 20 vol%. The HEAp/Al composites with 20 vol% HEAp content showed the maximum value with 3.57 g/cm3, which have an improvement of about 27% compared with unreinforced 7075Al matrix (about 2.81 g/cm3). Besides, the relative density has no obvious variation as to the improvement of HEAp content. In addition, all the HEAp/Al samples had a high relative density exceeding 99%.
Theoretically, the density of HEAp/Al composites follow the rule of mixture, which means that the theoretical density was decided by the volume fraction of reinforcement and matrix, the relation is shown as Equation (2):
pc = Vrpr + Vmpm
where, V and p refer to the volume fraction and density, subscript m, c, and r represent the matrix, composites, and reinforcement respectively. The theoretical density of HEAp and 7075Al is calculated by Equation (2) with the pHEA= 6.72 g/cm3 and pAl = 2.82 g/cm3, the theoretical values of HEAp/Al with 0, 5, 10, 15 and 20 vol% are 2.82, 3.04, 3.21, 3.41 and 3.59 g/cm3, which means the values were similar to the measured density tested by the Archimedes method. According to relevant reference [26], breaking of the oxide layer of particles and decrease of pores attributed to the mechanical and thermal effects during the sintering process can obtain a high relative density exceeding 96%. In this work, the high relative density larger than the former can demonstrate that the sintering process was reasonable and the carve defects were absent in the composites.

3.4. Hardness of HEAp/Al Composites

As one of the significant parameters of mechanical properties, hardness can well reflect the magnitude of plastic deformation resistance of composites. The Rockwell hardness values of HEAp/Al composites with different HEAp contents are shown in Figure 7. The hardness increases with the improvement of HEAp volume fraction, and reaches a maximum with the value of 84HRC when the volume fraction was up to 20 vol%. Compared with the unreinforced Al matrix (74HRC), the hardness of HEAp/Al composites with 5, 10, 15, and 20 vol% HEAp is improved by about 4%, 6.7%, 9.5%, and 13.5%, and the value is 77, 79, 81 and 84HRC, respectively. The improvement of Rockwell hardness of HEAp/Al is mainly attributed to the following reasons: (1) the hardness of HEAp is about 500HV [17], which is considerably larger than that of the 7075Al matrix (74HRC ≈ 80HV). The addition of the hardening phase not only bears mass load but also restrains the plastic deformation of the Al matrix, which means that the higher the reinforcement content, the higher the hardness; (2) the semi-coherent or incoherent interface between reinforcement and matrix inhibit the movement of dislocations in aluminum matrix; (3) increase of dislocation density at interface caused by the thermal expansion mismatch between HEAp and 7075Al matrix lead to difficulty in dislocation movement. Hence, the HEAp/Al composites have a better ability to resist plastic deformation than unreinforced Al matrix.

3.5. Mechanical Properties and Failure of HEAp/Al Composites

The flexural strength and fracture toughness of HEAp/Al composites with different HEAp volume fractions of 0, 5, 10, 15, and 20 vol% respectively are shown in Figure 8. It can be seen that the values of flexural strength and fracture toughness have a variation of increase at first and then decrease, and are higher than those of 7075Al matrix, which indicates that the HEAp possessed excellent strengthening and toughening effect on the mechanical properties of 7075Al matrix. The HEAp/Al composites with 10 vol% HEAp have the best flexural strength of 640 MPa and fracture toughness of 13.67 MPa·m1/2 compared with other HEAp/Al composites, which is improved by about 124.2% and 107.8% respectively compared with 7075Al matrix. Interestingly, the flexural strength and fracture toughness of HEAp/Al composites with 15 vol% HEAp is up to 582 MPa and 13.45 MPa·m1/2, which are slightly less than those of HEAp/Al composites with 10 vol% HEAp.
The fracture morphologies of HEAp/Al composites can reflect their failure mode variation with the improvement of HEAp content. As shown in Figure 9a, a large amount of dimples appears on the fracture surface with small-size appearing on fracture of 7075Al, this indicates that failure mode was essential of obvious ductile fracture characteristics. With the addition of HEAp reinforcements, the fractures become more uneven as the increase of HEAp content, as shown in Figure 9b–d. Moreover, two varieties of dimples with obviously different sizes appear on the fracture. The dimples with large size are formed because of the interfacial delamination of HEAp while the small-sized dimples are generated by the ductile fracture of 7075Al matrix. In addition to the formation of different size dimples, particle agglomeration can be observed on the fracture of HEAp/Al composites with 20% HEAp content (Figure 9d), which caused the matrix deficiency between HEAp.
The strengthening mechanisms of particles reinforced metals matrix composites mainly include dislocation strengthening behavior and load transfer effect [27]. Because of the rapid cooling rate of HEAp/Al from sintering temperature to room temperature, mismatch strain εCTE will be induced owing to the significant difference in thermal expansion coefficient between HEAp and 7075Al matrix. Then, geometrically necessary dislocation loops will be imposed around the surface of reinforcement to accommodate the thermal mismatch deformation. Hence, the number of dislocations loop increases as the improvement of HEAp volume fraction, in other words, high-density dislocation loops can restrain the crack initiation and propagation of microcracks. Besides, the metallurgical bonding interface between reinforcements and matrix improves the load transfer efficiency from 7075Al matrix to HEAp, and constrains the deformation of 7075Al matrix. These are reasons for the performance improvement of HEAp/Al composites. In comparison, the load transfer effect plays a greater role compared with dislocation strengthening behavior due to the incomparable size between HEAp and dislocation loops. Interestingly, Excessive content of reinforcement (20 vol% HEAp) lead to aggravating of stress concentration and microcrack initiation and propagation, while decrease dislocation density and load transfer efficiency, these means strengthening effect would be weakened, so that the mechanical properties of HEAp/Al composites with 20 vol% is lower than those of HEAp/Al composites with 10 vol% and 15 vol%.

4. Conclusions

  • FeCoCrNiAl high-entropy alloy particles (HEAp) reinforced 7075Al matrix composites (HEAp/Al) with dense microstructure and homogeneous distribution of reinforcement were fabricated by vacuum hot pressing sintering process at 580 °C, 30 MPa with 10 min holding time;
  • With the increase of HEAp volume fractions, the hardness of HEAp/Al composites increase and have a larger value compared with the 7075Al matrix. While flexural strength and fracture toughness of HEAp/Al composites increase first and then decrease. the HEAp/Al composites with HEAp volume fraction of 10 vol% show the highest maximum value of ~640 MPa and ~13.67 MPa·m1/2 and temperate density with the value of 3.19 g/cm3, respectively. The strengthening effect including load transfer effect and dislocation strengthening behavior increased with the improvement of HEAp content from 5 vol% to 15 vol%, while it was weakened when HEAp was up to 20 vol%.

Author Contributions

Conceptualization, C.G. and Q.M.; methodology, C.G.; composites-preparation, Q.W., M.W., H.F. and L.Z.; formal analysis, C.G.; investigation, C.G. and Q.M.; resources, Y.W.; writing—original draft preparation, C.G.; writing—review and editing, C.G.; supervision, Q.M.; project administration, Y.W.; funding acquisition, Q.M. and Y.W. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by Innovation Fund Project of Gansu Provincial Department of Education (Grant No. 2021A-030) and project supported by the National Natural Science Foundation of China (Grant No. 52162005).

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. The fabrication process of HEAp/Al composites.
Figure 1. The fabrication process of HEAp/Al composites.
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Figure 2. The XRD of unreinforced Al and HEAp/Al composites with 10 vol% HEAp.
Figure 2. The XRD of unreinforced Al and HEAp/Al composites with 10 vol% HEAp.
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Figure 3. Morphologies of HEAp/Al composites with different HEAp volume fraction; (a) 5 vol%; (b) 10 vol%; (c) 15 vol%; (d) 20 vol%.
Figure 3. Morphologies of HEAp/Al composites with different HEAp volume fraction; (a) 5 vol%; (b) 10 vol%; (c) 15 vol%; (d) 20 vol%.
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Figure 4. EDS mappings of interface between HEAp and 7075Al matrix.
Figure 4. EDS mappings of interface between HEAp and 7075Al matrix.
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Figure 5. (a) TEM of interface between HEAp and 7075Al matrix and (b) high magnification of interface microstructure3.4. Effects of HEAp Content on HEAp/Al Composites Density.
Figure 5. (a) TEM of interface between HEAp and 7075Al matrix and (b) high magnification of interface microstructure3.4. Effects of HEAp Content on HEAp/Al Composites Density.
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Figure 6. Density and relative density of HEAp/Al composites with different HEAp content.
Figure 6. Density and relative density of HEAp/Al composites with different HEAp content.
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Figure 7. Rockwell hardness of HEAp/Al composites with different HEAp content.
Figure 7. Rockwell hardness of HEAp/Al composites with different HEAp content.
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Figure 8. Flexural strength and fracture toughness of HEAp/Al composites with different HEAp volume fraction.
Figure 8. Flexural strength and fracture toughness of HEAp/Al composites with different HEAp volume fraction.
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Figure 9. Fractures of HEAp/Al composites with different HEAp content; (a) 0 vol% HEAp; (b) 5 vol% HEAp; (c) 10 vol% HEAp; (d) 20 vol% HEAp.
Figure 9. Fractures of HEAp/Al composites with different HEAp content; (a) 0 vol% HEAp; (b) 5 vol% HEAp; (c) 10 vol% HEAp; (d) 20 vol% HEAp.
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Gao, C.; Wang, Q.; Wei, M.; Fan, H.; Zhao, L.; Wei, Y.; Ma, Q. Effects of Reinforcement Volume Fraction on Mechanical Properties and Microstructures of 7075Al Matrix Composites Reinforced by FeCoCrNiAl High-Entropy Alloy Particles. Metals 2022, 12, 851. https://doi.org/10.3390/met12050851

AMA Style

Gao C, Wang Q, Wei M, Fan H, Zhao L, Wei Y, Ma Q. Effects of Reinforcement Volume Fraction on Mechanical Properties and Microstructures of 7075Al Matrix Composites Reinforced by FeCoCrNiAl High-Entropy Alloy Particles. Metals. 2022; 12(5):851. https://doi.org/10.3390/met12050851

Chicago/Turabian Style

Gao, Changqi, Qiaobo Wang, Mingyu Wei, Hongjing Fan, Libo Zhao, Yupeng Wei, and Qin Ma. 2022. "Effects of Reinforcement Volume Fraction on Mechanical Properties and Microstructures of 7075Al Matrix Composites Reinforced by FeCoCrNiAl High-Entropy Alloy Particles" Metals 12, no. 5: 851. https://doi.org/10.3390/met12050851

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