3.1. Microstructure
The optical micrographs of pure magnesium samples after extrusion and annealing are presented in Fig. 3. It is evident that the grain size is reduced after extrusion (Fig. <link rid="fig3">3</link>-a and 3-b) compared to that after annealing (Fig. <link rid="fig3">3</link>-c and 3-d). This phenomenon is due to recrystallization and grain growth during annealing.
The optical micrographs of the Mg-1% SiO2 composite samples at two different magnifications are depicted in Fig. 4. The figure highlights the comparison between the grain size observed after extrusion and the grain size observed after annealing. It is noteworthy that the inclusion of 1% of nanoparticles in the composite material appears to have a noticeable impact on the annealing process as it limits the growth of grains during the process. A comparison between Fig. 3 and Fig. 4 confirms that adding nanoparticles to the composite material significantly impacts the material's grain size.
Figures 5a-f depict the optical microscope images of pure magnesium and Mg-1% SiO2 composite after the extrusion process. The images suggest that the composite sample has a smaller average grain size when compared to the pure magnesium sample. The primary reason for this is the pinning of grain boundaries by nanoparticles, which inhibits the growth of grains.
Twinning is a mechanism of deformation in the hexagonal crystallographic lattice of magnesium. Figure 6 displays deformation twins that occur after the extrusion process. In this mechanism, a region of the atomic lattice is deformed so that it forms a mirror image relative to a twinning plane [17, 18]. These twins appear inside the grains and are visible as two parallel lines.
3.2. Texture of the extruded composite
The X-ray diffraction patterns for pure magnesium and composite samples after accumulative extrusion and annealing are presented in Fig. 7. The diffraction patterns observed at 2θ = 32°, 34° and 36° in the extruded magnesium and Mg-2% SiO2 samples correspond to the prismatic planes (10–10), basal planes (0002), and pyramidal planes (11 − 10), respectively, according to [13]. A comparison of pure magnesium X-ray diffraction patterns (Fig. 7a) shows that the basal planes in the extrusion direction have a higher peak intensity than those in the normal direction. It was observed that the pure magnesium is deformed in the direction in which the basal planes intersect, leading to the formation of a strong texture [10]. On annealing the pure magnesium samples, recrystallization occurs, which replaces deformed grains with recrystallized grains, resulting in a weakening of the texture created by the extrusion process and a decrease in the intensity of basal planes in the extrusion direction [14, 19]. It is worth noting that the pyramidal planes' peak intensity in the ND diagram of pure magnesium is higher than that of the prismatic and basal planes. Moreover, when recrystallization occurs, the intensity of the basal planes in the ND diagram decreases, indicating the texture's weakening [14].
The results from Fig. 7b indicate that the pyramidal planes have the highest peak intensity in the ND of the composite samples. The presence of nanoparticles in the composite leads to a decrease in the intensity of the basal planes [20, 21]. The maximum peak intensity of the composite in the ED direction belongs to the basal planes, and with the presence of nanoparticles, the peak intensity of the basal planes decreases. As a result, magnesium crystals exhibit a preferred orientation, which subsequently reduces the compressive stress asymmetry [9]. In general, it reduces the nucleation and development of twins, which leads to a decrease in the ultimate strength [9]. The inclusion of nanoparticles leads to a reduction in the peak intensity of the basal planes in the ED direction, causing a weakening of the basal texture in the composite relative to pure magnesium [13]. Figures 7c and 7d show that the peak intensity of the basal planes decreases for the annealed Mg-2%SiO2 composite samples, indicating that recrystallization weakens the texture of the composites. Furthermore, the intensity of the basal plane peaks in the annealed Mg-1 wt.% SiO2 composite samples is significantly greater than that in the annealed pure magnesium. This can be attributed to the uniform distribution of 1wt.% nanoparticles in the grain boundaries, effectively preventing grain growth during annealing. These findings demonstrate that the texture of the composites is preserved even after the annealing process.
3.3. Compression test
Figure 8 illustrates the compression stress-strain curves of pure magnesium samples after undergoing extrusion and annealing processes along the ND and ED of the samples. The curves show that the elastic response of magnesium is different along these directions, indicating its anisotropic behavior in elastic deformation. According to Tromans [22], the elastic modulus in the base planes differs from that in the prismatic and pyramidal planes for a hexagonal close-packed crystal structure. For magnesium, the elastic modulus in the base planes is 50.8 GPa, while it is 45.5 GPa in the prismatic and pyramidal planes [22]. Since the intensity of the basal planes in the ED is less than that in the prismatic planes, the elastic modulus in the ED is smaller than that in the ND. The two different behaviors of pure magnesium in these loading directions are worth noting. When the stress-strain curve is applied along the ED direction, the nucleation of the tensile twin is activated. The deformation of twins leads to a preferred crystal orientation, and the basal planes align in a perpendicular direction to the loading direction. After further loading, the deformation of a strong basal texture (parallel to the loading direction) begins at a strain of about 0.08. This strain magnitude corresponds to the maximum shear stress produced by the tensile twins. Thus, it is predicted that most grains in these samples will form a basal texture due to the tensile twins at a strain of approximately 0.08 [20, 23].
As can be seen from Fig. 8a, the loading direction parallel to the c-axis of the crystalline structure (ND) results in prevention of the slip in the basal planes. At high temperatures, pyramidal and prismatic systems can be activated, leading to the nucleation and growth of contraction twins [13, 24]. Due to the critical shear stress, the possibility of activation of the contraction twins is higher than that of the tensile ones, resulting in significant work-hardening at the beginning of the ND stress-strain curve. This work-hardening includes three regions, as reported elsewhere [23, 25]: elastic deformation, plastic deformation with activation of contraction twins, and fracture.
The stress-strain curves for pure magnesium after annealing are displayed in Fig. 8b. The X-ray diffraction patterns of pure magnesium in Fig. 7a indicate that the basal planes in the ED and ND directions have a higher peak intensity compared to other planes, signifying the texture generated in the samples' extrusion process. In contrast, the X-ray diffraction patterns of pure magnesium after the annealing process (Fig. 7a) demonstrate that the peak intensity of the basal planes has decreased in the ED and ND directions due to the texture weakening caused by the annealing process. Furthermore, Fig. 8b indicates that the samples' yield strength has decreased due to the annealing process. The stress-strain curves in Fig. 8b show that the grains increased in size during the annealing process of the samples. This caused tension twins to form when the sample was compressed. As a result, the ultimate strength of the annealed sample increased compared to the non-annealed sample [17, 23].
In Fig. 8 the curve of the ND similar to many ductile metals. However, the curve of the ED is quite different and can be divided into four regions [24, 26, 27]:
1- elastic deformation
2- plastic deformation by dislocations slip in the basal planes and tensile twin mechanisms.
3- plastic deformation with nucleation, growth and multiplication of tensile twins, interaction of dislocations with tensile twins and increase of hardening rate.
4- instability and fracture
When a load is applied along the ED direction, deformation in magnesium is initiated by the slip of dislocations on the basal planes. Based on Table 2, the critical resolved shear stress required for activating these systems is approximately 1 MPa. Therefore, deformation commences with the movement of dislocations. Subsequently, as the applied load increases, the shear stress increases, and the tensile twin mechanism comes into action. With the nucleation and growth of the tensile twins, the grains become finer, leading to an increase in the material strength according to the Hall-Petch law [17, 28].
Table 2
Room temperature critical resolved shear stress for the main deformation modes measured in single crystals of pure magnesium [28]
Deformation mode
|
Critical shear stress (MPa)
|
Basal < 𝑎 > slip
|
0.5-1
|
Prismatic < 𝑎 > slip
|
40–50
|
Pyramidal < 𝑐 + 𝑎 > slip
|
40–80
|
Tension twinning
|
2.4
|
Contraction twinning
|
115
|
Figure 9a displays a comparison of stress-strain curves between pure magnesium and nanocomposites along ND. Upon adding amorphous nanoparticles to the magnesium matrix, an enhancement in the yield strength and ductility is observed. This is attributed to the interaction between nanoparticles and dislocations, thus contributing to an increase in the strength of the nanocomposite. Additionally, the critical shear stress required to activate prismatic slip systems increases, which further strengthens the nanocomposite. In contrast, pure magnesium has a lower rate of work-hardening due to the absence of a reinforcing phase. Consequently, the improvement in the ductility of the nanocomposite can be attributed to the activation of the non-basal slip systems [13]. It is important to note that under compressive load, the dominant plastic deformation mechanism is twinning [28]. However, the addition of nanoparticles, while increasing strength, also limits the formation of twins. By adding 1wt.% of amorphous silica nanoparticles, an increase in both the yield strength and ductility is observed, while the ultimate strength decreases. Therefore, nanoparticles by being placed in the grain boundary, lead to an increase in yield strength and increase ductility while limit basal slip systems and activation of non-basal systems [29, 30].
Figure 9b shows comparison between stress-strain curves of the nanocomposites and pure magnesium samples along ED. The graph reveals that the addition of 1wt.% of amorphous nanoparticles to the magnesium matrix results in an increase in yield strength and strength within the strain range of 0.02–0.13, while the ultimate compressive strength decreases. The uniform dispersion of the nanoparticles in the microstructure during the extrusion process reduces the grain size [14]. According to Hall-Petch relationship, the yield strength increases as the grain size decreases [17, 31]. In addition, the presence of nanoparticles weakens the texture, leading to a decrease in the work-hardening rate and ultimate strength in the composite compared to the monolithic sample [13].
Figures 9c and d display how annealing affects the stress-strain response of pure magnesium and nanocomposite samples. The annealing process reduces the difference in the elastic modulus in different directions. This is due the fact that the annealing process weakens the texture [14, 24]. The Figure also indicates that the ultimate strength of the nanocomposite specimen increases after annealing. This increase may be due to the prevention of grain growth by the nanoparticles in the nanocomposites during the annealing process. As a result, the speed of the twin nucleation decreases, and the presence of nanoparticles limits the dislocation movement. [14, 32]. Both mechanisms increase the ultimate strength [33, 34]. Tables 3 and 4 list the mechanical properties of the nanocomposites and pure magnesium after extrusion and annealing, respectively. The tables show that nanocomposite specimen's yield strength, ductility, and ultimate strength have increased after the AE process and annealing.
Table 3
Mechanical properties of Mg-SiO2 nanocomposite and pure magnesium after the AE process
Sample
|
Yield strength (MPa)
|
Ultimate compression strength (MPa)
|
Elongation (%)
|
Pure Mg (ED)
|
49 ± 3
|
260 ± 3
|
-
|
Pure Mg (ND)
|
25 ± 3
|
235 ± 4
|
-
|
Mg-1%SiO2 (ED)
|
96 ± 2
|
240 ± 3
|
5
|
Mg-1%SiO2 (ND)
|
48 ± 3
|
215 ± 2
|
45
|
Mg-2%SiO2 (ED)
|
80 ± 3
|
230 ± 3
|
11
|
Mg-2%SiO2 (ND)
|
46 ± 2
|
220 ± 3
|
38
|
Table 4
Mechanical properties of annealed Mg-SiO2 nanocomposite and pure magnesium samples
Sample
|
Yield strength (MPa)
|
Ultimate compression strength (MPa)
|
Elongation (%)
|
Pure Mg (ED)
|
27 ± 3
|
250 ± 3
|
-
|
Pure Mg (ND)
|
23 ± 3
|
248 ± 4
|
-
|
Mg-1%SiO2 (ED)
|
47 ± 2
|
270 ± 3
|
5
|
Mg-1%SiO2 (ND)
|
42 ± 3
|
270 ± 2
|
40
|
Mg-2%SiO2 (ED)
|
40 ± 3
|
230 ± 3
|
4
|
Mg-2%SiO2 (ND)
|
39 ± 2
|
255 ± 3
|
25
|
3.4. Hardness
Numerous techniques have been proposed to enhance the mechanical properties of magnesium matrix composites. By analyzing the size and shape of the grains and the properties of the composite samples, it is possible to evaluate the effectiveness of the manufacturing process [9, 14, 35]. To assess the impact of the accumulative extrusion process on the hardness of the extruded materials, Brinell hardness was measured in the ND and TD planes for pure magnesium and nanocomposites samples. Figure 10 compares the hardness of the pure magnesium and nanocomposite samples after the extrusion and annealing processes. The hardness of the as-extruded pure magnesium increased from 35.1 Brinell to 40.6 Brinell in the Mg-2wt.%SiO2 nanocomposite, representing a 15.7% rise in hardness. This significant increase in hardness could be attributed to the presence of uniformly distributed nanoparticles in the magnesium matrix. During the AE process, the driving force of dynamic recrystallization increases, leading to more grain refinement. Therefore, AE is a highly effective solid-state process for dispersing nanoparticles in the matrix. Furthermore, the hardness of pure magnesium increased from 28.1 Brinell after annealing to 37.5 Brinell in the Mg-2wt.%SiO2 composite sample, indicating a 33.5% hike in hardness. This suggests that individual nanoparticles inhibited grain growth during recrystallization, leading to improved hardness.