Microstructures and Mechanical Properties of Nanocrystalline AZ31 Magnesium Alloy Powders with Submicron TiB2 Additions Prepared by Mechanical Milling

In this work, nanocrystalline AZ31 magnesium alloy powders, reinforced by submicron TiB2 particles, were prepared via mechanical milling. It was found that TiB2 particles stimulated the fracture and welding of AZ31/TiB2 powders, leading to the acceleration of the milling process. Meanwhile, the TiB2 particles were refined to submicron-scale size during the milling process, and their distribution was uniform in the Mg matrix. In addition, the matrix was significantly refined during the milling process, which was also accelerated by the TiB2 particles. The formation of grain boundary segregation layers also led to the weakened TiB2 peaks in the XRD patterns during the mechanical milling. The grain sizes of AZ31–2.5 wt % TiB2, AZ31–5 wt % TiB2 and AZ31–10 wt % TiB2 powders were refined to 53 nm, 37 nm and 23 nm, respectively, after milling for 110 h. Under the combined effect of the nanocrystalline matrix and the well-dispersed submicron TiB2 particles, the AZ31/TiB2 composites exhibited excellent micro-hardness. For the AZ31–10 wt % TiB2 composite, the micro-hardness was enhanced to 153 HV0.5.


Introduction
At present, the development of high-strength light alloys has been required to meet the light-weight requirements, which is of great significance for energy saving in structural applications [1]. As the lightest structural metallic materials, magnesium (Mg) alloys have favorable application prospects in the fields of aerospace, automobile, electronics and other industries, because of their low density, high specific stiffness and strength, and good shock absorption [2,3]. However, the technical challenge in the wide application of Mg alloys was their low mechanical properties, especially at elevated temperatures (>200 • C) [4][5][6]. In order to extend the structural application of Mg alloys, it is necessary to search for effective methods to further strengthen the commercial Mg alloys.
It is widely proposed that grain refinement is an important method of strengthening metallic materials, while the nanocrystalline (NC) and ultrafine-grained (UFG) materials can exhibit better mechanical properties when compared with conventional coarse-grained materials [7,8]. For Mg alloys,  Before mechanical milling, the AZ31 chips and TiB2 particles were mixed together with different TiB2 particle additions of 2.5 wt %, 5 wt % and 10 wt %, while each mixture was 10 g in weight. Then, the mixtures and stainless-steel balls (Ф 5 mm, Ф 8 mm, Ф 10 mm) were put into the milling pots, which were also filled with inert argon gas. The mechanical milling was executed by a QM-3SP4 type planetary ball milling machine (Nanjing NanDa Instrument Plant, Nanjing, China). Through the preparation experiment, the optimum milling parameters were determined, which were given as follows: the mass ratio of ball to powder was 60:1 and the shaft rotation was 300 rpm. Then, the AZ31/TiB2 composite powders were cold pressed into green compacts (Φ 10 mm) under pressure of 1500 MPa, in the atmosphere of high purity argon (99.9%). Moreover, the relative densities of those green compacts could reach above 95%, which were calculated through the Archimedes method. The micro-hardness of the green compacts was measured using an HVS-1000 tester (Shanghai Optical Instrument Factory, Shanghai, China), with the load of 500 g and loading time of 20 s. The green compacts were carefully polished before hardness measurements.
In addition, X-ray diffraction (XRD, Rigaku Utima IV, Rigaku corperation, Japan) was utilized to examine the as-milled composite powers, using Cu-Kα radiation (40 Kv,40 mA). According to the XRD results, the grain size of the matrix was calculated using Scherrer's equation [24]. In this study, the as-milled powders were directly used as scanning electron microscope (SEM) samples, which were observed using a FEI APREO scanning electron microscope (FEI Company, Hillsboro, USA). The samples for SEM observation were prepared in the glove box filled with high purity argon (99.9%) and kept in the sealed sample boxes. The back scattered electron (BSE) images were used to analyze the distribution of TiB2 particles in the matrix. Meanwhile, a JEM-200 EX transmission electron microscope (TEM, JEOL Ltd, Tokyo, Japan) was utilized to identify the grain size of the as- detected clearly, and no other phases were detected. In addition, all the materials were weighed and mixed in a glove box filled with high purity argon (99.9%), in order to avoid oxidation.  Before mechanical milling, the AZ31 chips and TiB2 particles were mixed together with different TiB2 particle additions of 2.5 wt %, 5 wt % and 10 wt %, while each mixture was 10 g in weight. Then, the mixtures and stainless-steel balls (Ф 5 mm, Ф 8 mm, Ф 10 mm) were put into the milling pots, which were also filled with inert argon gas. The mechanical milling was executed by a QM-3SP4 type planetary ball milling machine (Nanjing NanDa Instrument Plant, Nanjing, China). Through the preparation experiment, the optimum milling parameters were determined, which were given as follows: the mass ratio of ball to powder was 60:1 and the shaft rotation was 300 rpm. Then, the AZ31/TiB2 composite powders were cold pressed into green compacts (Φ 10 mm) under pressure of 1500 MPa, in the atmosphere of high purity argon (99.9%). Moreover, the relative densities of those green compacts could reach above 95%, which were calculated through the Archimedes method. The micro-hardness of the green compacts was measured using an HVS-1000 tester (Shanghai Optical Instrument Factory, Shanghai, China), with the load of 500 g and loading time of 20 s. The green compacts were carefully polished before hardness measurements.
In addition, X-ray diffraction (XRD, Rigaku Utima IV, Rigaku corperation, Japan) was utilized to examine the as-milled composite powers, using Cu-Kα radiation (40 Kv,40 mA). According to the XRD results, the grain size of the matrix was calculated using Scherrer's equation [24]. In this study, the as-milled powders were directly used as scanning electron microscope (SEM) samples, which were observed using a FEI APREO scanning electron microscope (FEI Company, Hillsboro, USA). The samples for SEM observation were prepared in the glove box filled with high purity argon (99.9%) and kept in the sealed sample boxes. The back scattered electron (BSE) images were used to analyze the distribution of TiB2 particles in the matrix. Meanwhile, a JEM-200 EX transmission electron microscope (TEM, JEOL Ltd, Tokyo, Japan) was utilized to identify the grain size of the as- In addition, X-ray diffraction (XRD, Rigaku Utima IV, Rigaku corperation, Japan) was utilized to examine the as-milled composite powers, using Cu-Kα radiation (40 Kv,40 mA). According to the XRD results, the grain size of the matrix was calculated using Scherrer's equation [24]. In this study, the as-milled powders were directly used as scanning electron microscope (SEM) samples, which were observed using a FEI APREO scanning electron microscope (FEI Company, Hillsboro, USA). The samples for SEM observation were prepared in the glove box filled with high purity argon (99.9%) and kept in the sealed sample boxes. The back scattered electron (BSE) images were used to analyze the distribution of TiB 2 particles in the matrix. Meanwhile, a JEM-200 EX transmission electron microscope (TEM, JEOL Ltd, Tokyo, Japan) was utilized to identify the grain size of the as-milled AZ31 Mg alloy with different TiB 2 additions. The samples for TEM analysis were mechanically ground first, and polished to the thickness of 50 µm. Then, the polished TEM films were prepared using ion mill polishing.

Morphology Evolution of Powders
It is widely proposed that the MM process consists of repeated plastic deformation, cold welding and the fracturing of mixed powders through high-energy impact [25]. Meanwhile, the mechanical Crystals 2020, 10, 550 4 of 16 milling has significant influence on the particle size and particle shape of the as-milled powders. Figure 3 shows the morphological evolution of the composite powders, with a 5 wt % TiB 2 addition after milling for different times. From Figure 3a,b, it can be observed that many laminar powders were fractured from the AZ31 Mg alloy cutting chips. Meanwhile, it can also be observed that some laminar powders piled up, which was mainly attributed to the cold welding during the milling process. In other words, there was a competitive relationship between the fracture and welding of these powers. As the milling time was prolonged, the fracture mechanism became predominant, resulting in the decrease of particle size. After milling for 60 h, it can be seen that many particles were changed into a rod shape, as shown in Figure 3f. In addition, the length to width radio of particle size decreased gradually during the milling process, as shown in Figure 3c-k. Yu et al. [6] also reported a similar phenomenon for AZ61/Ti composite powders during mechanical milling. Such a phenomenon was the result of the severe plastic deformation of powders in the process of mechanical milling, induced by the high-speed impact of stainless-steel balls in the rotating milling pots [25]. After milling for 100 h, there was no significant change in the particle size, which reached a stable stage, as shown in Figure 3j-k. Meanwhile, the average particle size was refined to about 700 µm after milling for 110 h, and many particles became equiaxed. It should be noted that the particles with larger volume and higher hardness were prone to fracture, which was beneficial to equiaxation of the particles' shape [26]. Besides that, the occurrence of cold welding could also contribute to the appearance of equiaxed particles. It is widely proposed that the interfacial energy of powders would increase sharply with the emergence of a large number of small particles [27], which could promote the welding of powders. As shown in Figure 4, the content of the TiB2 additions also has a great influence on the morphologies of the powders. Combining Figure 3c,g,k and Figure 4, it can be found that both the length to width ratio and particle sizes decreased with the increasing content of TiB2 additions, and there were more equiaxed particles in the composite powders with high TiB2 additions. In other As shown in Figure 4, the content of the TiB 2 additions also has a great influence on the morphologies of the powders. Combining Figure 3c,g,k and Figure 4, it can be found that both the length to width ratio and particle sizes decreased with the increasing content of TiB 2 additions, and there were more equiaxed particles in the composite powders with high TiB 2 additions. In other words, the presence of hard TiB 2 additions could promote the fracturing of matrix particles, and accelerate the milling process, and they therefore acted as milling assistant agents. Meanwhile, the high stress concentration appeared as TiB 2 particles embedded in the matrix, which would promote the fracture of powders. Meanwhile, the reinforcement particles with high hardness significantly enhanced the local deformation of the matrix [28]. It can be inferred that the enhanced deformation caused by TiB 2 particles would stimulate the cold welding and fracture of powders, leading to the acceleration of the milling process.

Evolution of TiB2 Particles
As mentioned above, the TiB2 reinforcement has a positive effect on the refinement rate of powders during mechanical milling. Moreover, the characteristics of TiB2 particles are also very important for the properties of the composite materials, including the size of TiB2 particles and their distribution in matrix [29]. To investigate the evolution of TiB2 particles during mechanical milling, the BSE images of the AZ31/TiB2 powders were analyzed in detail. These images were taken from the flat parts in powders. Figure 5a-f shows BSE images of AZ31/TiB2 powders with 5 wt % TiB2 addition after milling for different times. Meanwhile, the EDS results of point A and point B marked in Figure  5a were also given, as shown in Figure 5g-h. According to the EDS result of point A, the gray area in

Evolution of TiB 2 Particles
As mentioned above, the TiB 2 reinforcement has a positive effect on the refinement rate of powders during mechanical milling. Moreover, the characteristics of TiB 2 particles are also very important for the properties of the composite materials, including the size of TiB 2 particles and their distribution in matrix [29]. To investigate the evolution of TiB 2 particles during mechanical milling, the BSE images of the AZ31/TiB 2 powders were analyzed in detail. These images were taken from the flat parts in powders. Figure 5a-f shows BSE images of AZ31/TiB 2 powders with 5 wt % TiB 2 addition after milling for different times. Meanwhile, the EDS results of point A and point B marked in Figure 5a were also given, as shown in Figure 5g-h. According to the EDS result of point A, the gray area in the BSE images was identified as AZ31Mg alloy. As for the EDS result of point B, there were Ti and B elements in the white particles, which were the components of TiB 2 . In other words, the white particles should be the TiB 2 additions. was uniform. With the increase in milling time, it is interesting to find that there were some big TiB2 particles around the crack, while the fine TiB2 particles uniformly dispersed in the Mg matrix, as shown in Figure 5d-f. In other words, the dispersed fine particles were easily entered into the matrix, which can promote the uniform distribution of reinforcing particles. Meanwhile, the big TiB2 particles seemed to be more tended towards promoting the fracture of the Mg matrix, due to the introduction of a high stress concentration. From Figure 5c-f, it can also be seen that the average size of the TiB2 particles was refined with the prolonging of milling time. The refinement of TiB2 particles was mainly attributed to the fracture mechanism, which was similar to the refinement of the matrix. Then, an increasing number of fine particles entered into the matrix, and the uniform distribution of TiB2 particles in the Mg matrix was gradually achieved. After milling for 110 h, the average size of TiB2 particles was refined to about 0.4 μm, which had reached submicron-scale. As reported, the homogeneous distribution of submicron-scale TiB2 particles could noticeably strengthen the matrix through the Orowan strengthening mechanism [30]. Besides that, not only was the size of TiB2 particles refined during mechanical milling, but the sharp edges of the TiB2 particles were also gradually eliminated, leading to a rounder morphology.  After milling for 10 h, a high quantity of TiB 2 particles assembled on the surface of matrix, and the distribution of TiB 2 particles exhibited a reunited state. As in Figure 5a, there was a typically large cluster, marked with the yellow ellipse region, which was mainly composed of TiB 2 particles. The formation of this large cluster was mainly caused by the inadequate milling. With the increasing Crystals 2020, 10, 550 7 of 16 milling time, cold welding and deformation occurred in the Mg matrix. In this case, these clusters between two or more matrix particles would be wrapped in the matrix at the instant of ball-collision, leading to the dispersion of clusters in the matrix. As shown in Figure 5b, there were also TiB 2 clusters after milling for 30 h, due to the existence of an agglomeration force between TiB 2 particles. Meanwhile, these TiB 2 clusters would also be gradually disintegrated by the high-energy collisions between the grinding balls and powders. After milling for 50 h, it can be observed that there were few clusters of TiB 2 particles in matrix, as shown in Figure 5c, and the distribution of TiB 2 particles was uniform. With the increase in milling time, it is interesting to find that there were some big TiB 2 particles around the crack, while the fine TiB 2 particles uniformly dispersed in the Mg matrix, as shown in Figure 5d-f. In other words, the dispersed fine particles were easily entered into the matrix, which can promote the uniform distribution of reinforcing particles. Meanwhile, the big TiB 2 particles seemed to be more tended towards promoting the fracture of the Mg matrix, due to the introduction of a high stress concentration. From Figure 5c-f, it can also be seen that the average size of the TiB 2 particles was refined with the prolonging of milling time. The refinement of TiB 2 particles was mainly attributed to the fracture mechanism, which was similar to the refinement of the matrix. Then, an increasing number of fine particles entered into the matrix, and the uniform distribution of TiB 2 particles in the Mg matrix was gradually achieved. After milling for 110 h, the average size of TiB 2 particles was refined to about 0.4 µm, which had reached submicron-scale. As reported, the homogeneous distribution of submicron-scale TiB 2 particles could noticeably strengthen the matrix through the Orowan strengthening mechanism [30]. Besides that, not only was the size of TiB 2 particles refined during mechanical milling, but the sharp edges of the TiB 2 particles were also gradually eliminated, leading to a rounder morphology.
Based on the BSE images, it was found that 5 wt % TiB 2 particles of uniform size were uniformly distributed in the matrix after milling for 110 h. In order to further confirm the distribution at the element scale, the EDS maps of Mg, Ti, Al, Mn and Zn were characterized, as shown in Figure 6. It should be noted that all the Ti element in the EDS maps existed in the TiB 2 particles, which can be confirmed by the XRD analysis shown in Section 3.3. After milling for 110 h, the Ti element was uniformly distributed in the Mg matrix, as shown in Figure 6c, indicating the uniform distribution of TiB 2 particles. From Figure 6d-f, it can be observed that most of the Al, Mn and Zn elements were homogeneously dissolved into the Mg matrix. However, there were also some Al element existing in the Mg 17 Al 12 phase, and there were also intermetallic compounds or solid solutions of Mn in the matrix after milling for 110 h, which are highlighted by the ellipse regions.  Based on the BSE images, it was found that 5 wt % TiB2 particles of uniform size were uniformly distributed in the matrix after milling for 110 h. In order to further confirm the distribution at the element scale, the EDS maps of Mg, Ti, Al, Mn and Zn were characterized, as shown in Figure 6. It should be noted that all the Ti element in the EDS maps existed in the TiB2 particles, which can be   Figure 7 shows the XRD patterns of AZ31/TiB 2 composite powders with different TiB 2 additions after milling for different times. According to the result of XRD, the appearance of Mg and TiB 2 peaks can be clearly observed. However, it was very difficult to find Mg 17 Al 12 peaks in the XRD patterns of the AZ31/TiB 2 composite powders after mechanical milling, which was very similar to the other investigations [6,31]. Such a phenomenon was mainly owing to the decomposition of the Mg 17 Al 12 phase and the dissolving of Al into the Mg matrix during the milling process [31]. In addition, there were no other new phases detected in the XRD patterns after milling for different times, indicating that the TiB 2 particles did not react with the matrix during the milling process. Simultaneously, the diffraction intensity of the Mg peaks decreased with the increasing milling time, while the full width was attained at half the maximum of the Mg peaks' increase. Such a phenomenon was closely related to the refinement of grain size [24]. Meanwhile, the grain size can be approximated from the XRD data by using the following formula [24]:

XRD Analysis
where D is the grain size, k is the Scherrer constant, λ is the wavelength of the radiation, θ is the Bragg angle, and β f C can be calculated from the ratio of the Cauchy integral's breadth.
Crystals 2020, 10, x FOR PEER REVIEW 9 of 17 phase and the dissolving of Al into the Mg matrix during the milling process [31]. In addition, there were no other new phases detected in the XRD patterns after milling for different times, indicating that the TiB2 particles did not react with the matrix during the milling process. Simultaneously, the diffraction intensity of the Mg peaks decreased with the increasing milling time, while the full width was attained at half the maximum of the Mg peaks' increase. Such a phenomenon was closely related to the refinement of grain size [24]. Meanwhile, the grain size can be approximated from the XRD data by using the following formula [24]: where D is the grain size, k is the Scherrer constant, λ is the wavelength of the radiation, θ is the Bragg angle, and f C β can be calculated from the ratio of the Cauchy integral's breadth.   Figure 8 shows the grain size of the Mg matrix in milled composite materials, which was calculated by Equation (1). It can be observed that the grain size decreased with the increase of milling time, and there were three stages for the refinement of the grain size. In the initial milling stage, the grain refinement was rapid, and the grain size of the Mg matrix with different TiB2 additions was refined to below 150 nm after milling for 50 h. During the initial milling stage, the composite powders suffered repeated plastic deformations with high strain rates, resulting in the increasing dislocation density. When the dislocation density reached a critical value, the grain broke up into sub-grains separated by low angle grain boundaries [31], leading to the rapid refinement of Mg grains. With further milling, the grain refining would promote the generation of a lot of new grain boundaries. As a result, the subsequent refining required a larger critical dislocation density and more energy. However, the input energy was constant during the milling process. Therefore, the grain refinement rate slowed down during the middle stage. It can be found that the grain size of the Mg matrix, with  Figure 8 shows the grain size of the Mg matrix in milled composite materials, which was calculated by Equation (1). It can be observed that the grain size decreased with the increase of milling time, and there were three stages for the refinement of the grain size. In the initial milling stage, the grain refinement was rapid, and the grain size of the Mg matrix with different TiB 2 additions was refined to below 150 nm after milling for 50 h. During the initial milling stage, the composite powders suffered repeated plastic deformations with high strain rates, resulting in the increasing dislocation density. When the dislocation density reached a critical value, the grain broke up into sub-grains separated by low angle grain boundaries [31], leading to the rapid refinement of Mg grains. With further milling, the grain refining would promote the generation of a lot of new grain boundaries. As a result, the subsequent refining required a larger critical dislocation density and more energy. However, the input energy was constant during the milling process. Therefore, the grain refinement rate slowed down during the middle stage. It can be found that the grain size of the Mg matrix, with different TiB 2 additions, was refined to below 100 nm after milling for 70 h. In the last milling stage, the grain refinement rate decreased significantly, and reached a relatively stable stage. Such a phenomenon was mainly attributed to the dynamic balance between grain refinement and grain growth caused by the thermal effect. It should be noted that there was a temperature rise in the composite powders during the milling process, because of the intense impact between the grinding balls and the milling pots. Meanwhile, the temperature rise would provide favorable conditions for grain growth, and hinder grain refinement. After milling for 110 h, the grain sizes of the Mg matrices in the AZ31/TiB 2 composite powders with 2.5 wt %, 5 wt % and 10 wt % TiB 2 additions were refined to 58 nm, 39 nm and 27 nm, respectively.
From Figure 8, it also can be deduced that the grain refinement rate of the Mg matrix increased with the increasing TiB 2 additions. In other words, the grain refinement of the matrix during mechanical milling was accelerated by the TiB 2 additions. The pinning effect of TiB 2 particles can hinder the migration of grain boundaries and dislocations, which could inhibit the grain growth during the milling process. Besides that, the occurrence of TiB 2 particles could accelerate the dislocation pile-up. Thus, the dislocation density of the composite powders increased with the increasing TiB 2 additions, which could promote the grain refinement of the Mg matrix during the milling process.
Besides that, it is interesting to find that the TiB 2 peaks became weaker with the increasing milling time, and almost disappeared after 110 hours of milling, as shown in Figure 7. Such a phenomenon has also been recently observed in Cu-Ag alloys [32], steels [33] and doped ZnO [34], and it was closely related to grain boundary segregation effects. As mentioned in Figure 8, the Mg matrices were gradually refined to a nanocrystalline state with the increasing milling times, and contained a lot of grain boundaries. The grain boundary segregation layers formed where the Ti and B atoms were hidden. In other words, the formation of grain boundary segregation layers led to weakened TiB 2 peaks during the mechanical milling.   Figure 8 shows the grain size of the Mg matrix in milled composite materials, which was calculated by Equation (1). It can be observed that the grain size decreased with the increase of milling time, and there were three stages for the refinement of the grain size. In the initial milling stage, the grain refinement was rapid, and the grain size of the Mg matrix with different TiB2 additions was refined to below 150 nm after milling for 50 h. During the initial milling stage, the composite powders suffered repeated plastic deformations with high strain rates, resulting in the increasing dislocation density. When the dislocation density reached a critical value, the grain broke up into sub-grains separated by low angle grain boundaries [31], leading to the rapid refinement of Mg grains. With further milling, the grain refining would promote the generation of a lot of new grain boundaries. As a result, the subsequent refining required a larger critical dislocation density and more energy. However, the input energy was constant during the milling process. Therefore, the grain refinement rate slowed down during the middle stage. It can be found that the grain size of the Mg matrix, with

TEM Analysis
As mentioned above, the milled AZ31/TiB 2 composite powders were cold pressed into green compacts, which were utilized for TEM observation. It should be noted that the TEM analysis could directly reveal the structure of nanocrystalline Mg matrices. Figure 8 shows the TEM images and corresponding grain size distributions of AZ31/TiB 2 composite powders, with different TiB 2 additions and after milling for 110 h. As shown in Figure 9a, it can be confirmed that the matrix phase was Mg by indexing the rings of the diffracted spots taken from the matrix grains. As shown in Figure 9b, the Mg matrix with 2.5 wt % TiB 2 particles had been refined to the nano-structure state after milling for 110 h, and most of the grains ranged from 31 to 79 nm. The average size of the Mg matrix was 53 nm, which was very close to the result calculated by Scherrer's formula (58 nm). With the increase of TiB 2 particles, the pinning effect of TiB 2 particles in the matrix was further enhanced, while the dislocation pile-up was also accelerated. As a result, the grain size was further refined with the increase of TiB 2 particles. From Figure 9c

Hardness Analysis
The mechanical performance of the milled AZ31/TiB2 composite powders was evaluated by micro-hardness testing. Figure 10 shows the micro-hardness of the as-cast AZ31 Mg alloy and asmilled AZ31/TiB2 composites after milling for 110 h. It can be noted that the micro-hardness of the AZ31/TiB2 composites was much greater than that of the as-cast AZ31 Mg alloy, which also increased with the increasing TiB2 additions. For the AZ31-10 wt %TiB2 composite, its micro-hardness was enhanced to 153 HV0.5. There were three main reasons for the significant increase in the microhardness of the AZ31/TiB2 composites. The first one was grain boundary strengthening, which was closely related to the refinement of the Mg matrix. It has been reported that grain boundary strengthening can be calculated by the following formula [9,35,36]: where kγ is the Hall-Petch coefficient, and d is the mean grain size. After milling for 110 h, the grain size of the Mg matrix in the AZ31/TiB2 composite powders was refined to nanocrystalline scale, and it was further refined with the increasing TiB2 additions. The nanocrystalline matrix makes a

Hardness Analysis
The mechanical performance of the milled AZ31/TiB 2 composite powders was evaluated by micro-hardness testing. Figure 10 shows the micro-hardness of the as-cast AZ31 Mg alloy and as-milled AZ31/TiB 2 composites after milling for 110 h. It can be noted that the micro-hardness of the AZ31/TiB 2 composites was much greater than that of the as-cast AZ31 Mg alloy, which also increased with the increasing TiB 2 additions. For the AZ31-10 wt %TiB 2 composite, its micro-hardness was enhanced to 153 HV0.5. There were three main reasons for the significant increase in the micro-hardness of the AZ31/TiB 2 composites. The first one was grain boundary strengthening, which was closely related to the refinement of the Mg matrix. It has been reported that grain boundary strengthening can be calculated by the following formula [9,35,36]: where k γ is the Hall-Petch coefficient, and d is the mean grain size. After milling for 110 h, the grain size of the Mg matrix in the AZ31/TiB 2 composite powders was refined to nanocrystalline scale, and it was further refined with the increasing TiB 2 additions. The nanocrystalline matrix makes a great contribution to the improvement of micro-hardness. The second reason was the load-bearing effects of submicron TiB 2 particles, which were much harder than the Mg matrix. The hard submicron TiB 2 particles would bear the load transferred from the Mg matrix, which could effectively enhance the micro-hardness of the composites. Meanwhile, it should be noticed that the load-bearing effects were improved with the increasing content of reinforcements [37]. In other words, the load-bearing effects of the AZ31/TiB 2 composites could be enhanced by increasing the TiB 2 additions. On the other hand, the submicron TiB 2 particles would give rise to Orowan strengthening, which was the third reason for the improvement of micro-hardness. The well-dispersed submicron TiB 2 particles could limit the migration of dislocations, and cause the remarkable strengthening.
Crystals 2020, 10, x FOR PEER REVIEW 13 of 17 great contribution to the improvement of micro-hardness. The second reason was the load-bearing effects of submicron TiB2 particles, which were much harder than the Mg matrix. The hard submicron TiB2 particles would bear the load transferred from the Mg matrix, which could effectively enhance the micro-hardness of the composites. Meanwhile, it should be noticed that the load-bearing effects were improved with the increasing content of reinforcements [37]. In other words, the load-bearing effects of the AZ31/TiB2 composites could be enhanced by increasing the TiB2 additions. On the other hand, the submicron TiB2 particles would give rise to Orowan strengthening, which was the third reason for the improvement of micro-hardness. The well-dispersed submicron TiB2 particles could limit the migration of dislocations, and cause the remarkable strengthening. A comparison of the micro-hardness and grain sizes of various Mg alloys was carried out, as shown in Figure 11. The preparation processing included high-pressure torsion (HPT), spray-formed processing (SFP), disintegrated melt deposition (DMD), extrusion (ES), friction stir processing (FSP) and mechanical milling (MM). As can be concluded by the data comparison, the AZ31-10 wt % TiB2 composite in this study exhibited a competitive micro-hardness among the other Mg alloys that have been referred to, and it possessed the smallest grain size. The nanocrystalline matrix and the welldispersed submicron TiB2 particles made great contributions to the mechanical performance of the AZ31/TiB2 composite. From the comparison, it also can be concluded that MM was a feasible process for preparing TiB2 particles to reinforce the Mg alloy with high micro-hardness. A comparison of the micro-hardness and grain sizes of various Mg alloys was carried out, as shown in Figure 11. The preparation processing included high-pressure torsion (HPT), spray-formed processing (SFP), disintegrated melt deposition (DMD), extrusion (ES), friction stir processing (FSP) and mechanical milling (MM). As can be concluded by the data comparison, the AZ31-10 wt % TiB 2 composite in this study exhibited a competitive micro-hardness among the other Mg alloys that have been referred to, and it possessed the smallest grain size. The nanocrystalline matrix and the well-dispersed submicron TiB 2 particles made great contributions to the mechanical performance of the AZ31/TiB 2 composite. From the comparison, it also can be concluded that MM was a feasible process for preparing TiB 2 particles to reinforce the Mg alloy with high micro-hardness.