Aging Behavior of Aluminum Alloy 6082 Subjected to Friction Stir Processing

: The present work examined the effect of artiﬁcial aging on the microstructure, texture, and hardness homogeneity in aluminum alloy AA6082 subjected to friction stir processing (FSP). Aging was applied to FSP samples at three different temperatures (150 ◦ C, 175 ◦ C, and 200 ◦ C) for a period of 1 h, 6 h, and 12 h. Microstructure analysis using optical Microscopy (OM) and Electron Back-Scattered Diffraction (EBSD) indicated that FSP produced ﬁne equiaxed grains, with an average grain size of 6.5 µ m, in the stir zone (SZ) due to dynamic recrystallization. Aging was shown to result in additional grain reﬁnement in the SZ due to the occurrence of recovery and recrystallization with either increasing aging temperature and/or aging time. An optimum average grain size of 3–4 µ m was obtained in the SZ by applying aging at 175 ◦ C. This was accompanied by an increase in the fraction of high-angle grain boundaries. FSP provided a simple shear texture with a major component of B ﬁber. Increasing aging temperature and/or time resulted in the formation of recrystallization texture of a Cube orientation. In addition, Vickers microhardness was evaluated for the FSP sample, indicating a softening in the SZ due to the dissolution of the hardening precipitates. Compared to other aging temperatures, aging at 175 ◦ C resulted in maximum hardness recovery (90 Hv) to the initial value of base metal (92.5 Hv). The hardness recovery is most likely attributed to the uniform distribution of ﬁne hardening precipitates in the SZ when increasing the aging time to 12 h. etched at ambient temperature for about 6 min with an extended Flick’s reagent consisting of 1.5 parts of HCl, one part of HF, and nine parts of distilled water. The microstructure was further analyzed using a metallurgical microscope (AxioImager A1M, ZEISS, Oberkochen, Germany). A microetchant of Weck’s reagent was used to reveal grain boundaries, consisting of 100 mL distilled water, 4 gm potassium permanganate, and 1gm sodium hydroxide. precipitate hardening effect in the ultrafine-grained material. In addition, other studies examined the effect of post annealing on precipitation and microstructural evolution in AA6082 subjected to severe rolling reductions [33,34]. It was reported that at a low annealing temperature of 150 °C, the formation of new subgrains occurred with an increase in the faction of HAGBs. At higher annealing


Introduction
Friction stir processing (FSP) has been used in the last two decades as an effective surface modification method for grain refinement in metals, particularly for aluminum alloys [1,2]. FSP was originally developed from the principle of friction stir welding (FSW), which has been utilized as a solid state joining technique [3]. The heat input caused by the friction between the FSP tool shoulder and the surface of the material, combined with the stirring action of the tool pin, results in grain refinement in the stir zone (SZ) due to the intensive plastic deformation. The SZ is commonly characterized by a fine and equiaxed grain structure with predominant high-angle grain boundaries (HAGBs), which is generally attributed to dynamic recrystallization and the break-up of constituent particles [2]. Next to the SZ, a narrow transition region known as the thermo-mechanically affected zone (TMAZ) is formed, followed by the heat affected zone (HAZ), and finally the unaffected base metal (BM). The grain refinement by FSP has been shown to enhance several properties, including strength, ductility, toughness, and corrosion resistance [4].
Several works have examined the effect of microstructural refinement by FSP/FSW on 6000 series aluminum alloys [5][6][7][8][9][10][11][12]. These heat-treatable series have a good weight-to-strength ratio, combined with excellent corrosion resistance and ease of formability [13]. They are heavily utilized in architecture and structural applications. The 6000 series consists of two major alloying elements: silicon (Si)

Materials and Methods
Aluminum alloy 6082 (Industrial Metal Center Company, Shuwaikh, Kuwait) plates were received in a hot rolled condition. The aluminum alloy has a chemical composition (in wt. %) of 1.03 Si, 0.76 Mg, 0.53 Mn, and 0.21 Fe, with minor amounts of Ti, Cu, Ni, Va, Zn, and Zr. The dimensions of the FSP plates were 150 mm × 125 mm × 13 mm, as schematically illustrated in Figure 1a. FSP specimens were sectioned perpendicular to the rolling direction. The FSP tool material is made of heat-treated H13 steel; it has a shoulder of 25 mm in diameter and a 4 mm long pin with a 4 mm diameter. FSP of single pass was conducted using a vertical milling machine with a constant tool rotating rate of 1200 rpm and travel speed of 150 mm/min. Figure 1a schematically illustrates FSP of AA6082 plates, where WD, TD, and ND denote the processing, transverse, and normal directions of the plate, respectively. A post heat treatment of artificial aging was carried out on the FSP samples using three aging temperatures of 150 • C, 175 • C, and 200 • C. For each temperature, three aging periods of 1 h, 6 h, and 12 h were utilized. All aging treatments were applied to the FSP samples using an electric muffle furnace (JSMF-270T, JSR, Gongju, Korea). Metallographic samples were prepared for a microstructure evaluation of the processed area in FSP samples. The metallographic samples were cut from the cross-section of FSP plates (ND-TD plane) and then ground and polished using standard metallography techniques. Microstructure assessment of the processed area was first made using a (Stemi 2000c, ZEISS, Oberkochen, Germany). To do that, the samples were chemically etched at ambient temperature for about 6 min with an extended Flick's reagent consisting of 1.5 parts of HCl, one part of HF, and nine parts of distilled water. The microstructure was further analyzed using a metallurgical microscope (AxioImager A1M, ZEISS, Oberkochen, Germany). A microetchant of Weck's reagent was used to reveal grain boundaries, consisting of 100 mL distilled water, 4 gm potassium permanganate, and 1gm sodium hydroxide. Particle size analysis for the intermetallic phases within the SZ was also conducted using ImageJ, an automated image analysis system [17]. Further assessment of the microstructure development in the SZ was carried out using the Electron Back-Scattered Diffraction (EBSD) technique. The EBSD measurements were conducted with an SEM (7001F-JSM, JEOL, Tokyo, Japan) equipped with an EBSD system (Aztec, Oxford, High Wycombe, UK). Samples were prepared by using an electro-polishing unit (LectroPol-5, Struers, Ballerup, Denmark) with an electrolyte containing 700 mL ethanol, 100 mL 2-butoxyethanol, 120 mL water, and 80 mL perchloric acid. EBSD measurements were made to assess the microstructure refinement and texture evolution in the processed area, evaluating grain size, grain boundary misorientation distribution, and pole figures. EBSD maps were acquired with an area of 225 × 175 μm 2 with a step size of 0.1 to 0.3 μm. Depending on aging temperature and time, between nearly 750 and 1500 grains were analyzed for each EBSD map. This large number of grains allowed an adequate evaluation of microstructure and texture development. In addition, the critical misorientation angle used to discriminate grains from Metallographic samples were prepared for a microstructure evaluation of the processed area in FSP samples. The metallographic samples were cut from the cross-section of FSP plates (ND-TD plane) and then ground and polished using standard metallography techniques. Microstructure assessment of the processed area was first made using a (Stemi 2000c, ZEISS, Oberkochen, Germany). To do that, the samples were chemically etched at ambient temperature for about 6 min with an extended Flick's reagent consisting of 1.5 parts of HCl, one part of HF, and nine parts of distilled water. The microstructure was further analyzed using a metallurgical microscope (AxioImager A1M, ZEISS, Oberkochen, Germany). A microetchant of Weck's reagent was used to reveal grain boundaries, consisting of 100 mL distilled water, 4 gm potassium permanganate, and 1gm sodium hydroxide. Particle size analysis for the intermetallic phases within the SZ was also conducted using ImageJ, an automated image analysis system [17]. Further assessment of the microstructure development in the SZ was carried out using the Electron Back-Scattered Diffraction (EBSD) technique. The EBSD measurements were conducted with an SEM (7001F-JSM, JEOL, Tokyo, Japan) equipped with an EBSD system (Aztec, Oxford, High Wycombe, UK). Samples were prepared by using an electro-polishing unit (LectroPol-5, Struers, Ballerup, Denmark) with an electrolyte containing 700 mL ethanol, 100 mL 2-butoxyethanol, 120 mL water, and 80 mL perchloric acid. EBSD measurements were made to assess the microstructure refinement and texture evolution in the processed area, evaluating grain size, grain boundary misorientation distribution, and pole figures. EBSD maps were acquired with an area of 225 × 175 µm 2 with a step size of 0.1 to 0.3 µm. Depending on aging temperature and time, between nearly 750 and 1500 grains were analyzed for each EBSD map. This large number of grains allowed an adequate evaluation of microstructure and texture development. In addition, the critical misorientation angle used to discriminate grains from substructures was set to 10 • . The average grain size was calculated according to ASTM: E112, using an average intercept method program available with the EBSD software. Further examination of the texture development in the SZ was also made by X-ray diffraction (XRD). The measurements were carried out by a diffractometer (model: Bruker, D8 Advance, Billerica, MA, USA) using Cu Kα radiation at a scan rate of 0.02 • per second.
Additionally, hardness indentations were made using a Vickers microhardness tester (Micromet 4, Buehler, Lake Bluff, IL, USA). As schematically described in Figure 1b, the indentations were made horizontally on the cross-section of the processed plate at sections A-A, B-B, and C-C, i.e., 0.5, 1.5, and 2.5 mm from the processed surface, respectively. Indentations on each line were made in an increment of 0.5 mm and using a load of 200 gf and dwell time of 15 s. Figure 2 demonstrates a low-magnification view of the transverse cross section, i.e., the ND-TD plane, of the FSP plate. Three distinct zones can be identified: SZ, TMAZ, and BM. No distinct HAZ was found for the FSP samples. In general, a basin-shape of the processed area was produced for all FSP samples. The microstructure in the SZ has been refined into very small grains. The TMAZ is very narrow, about 100-200 µm, resulting in a sharp transition from a fine-grained SZ microstructure into a lamellar-type structure of flat elongated grains in the BM. The microstructure development in the BM is due to the use of hot rolling on the as-received AA6082 plates. In addition, no porosity or defects were generally detected in the processed area for all examined FSP samples. substructures was set to 10°. The average grain size was calculated according to ASTM: E112, using an average intercept method program available with the EBSD software. Further examination of the texture development in the SZ was also made by X-ray diffraction (XRD). The measurements were carried out by a diffractometer (model: Bruker, D8 Advance, Billerica, MA, USA) using Cu Kα radiation at a scan rate of 0.02° per second. Additionally, hardness indentations were made using a Vickers microhardness tester (Micromet 4, Buehler, Lake Bluff, IL, USA). As schematically described in Figure 1b, the indentations were made horizontally on the cross-section of the processed plate at sections A-A, B-B, and C-C, i.e., 0.5, 1.5, and 2.5 mm from the processed surface, respectively. Indentations on each line were made in an increment of 0.5 mm and using a load of 200 gf and dwell time of 15 s. Figure 2 demonstrates a low-magnification view of the transverse cross section, i.e., the ND-TD plane, of the FSP plate. Three distinct zones can be identified: SZ, TMAZ, and BM. No distinct HAZ was found for the FSP samples. In general, a basin-shape of the processed area was produced for all FSP samples. The microstructure in the SZ has been refined into very small grains. The TMAZ is very narrow, about 100-200 μm, resulting in a sharp transition from a fine-grained SZ microstructure into a lamellar-type structure of flat elongated grains in the BM. The microstructure development in the BM is due to the use of hot rolling on the as-received AA6082 plates. In addition, no porosity or defects were generally detected in the processed area for all examined FSP samples.  The structure of BM shows a typical deformed structure developed by rolling. The deformed structure is shown to be a lamellar type and aligned with the rolling direction. Most of the grains in the BM are small, with an average size of less than 10 μm. It is also evident that FSP produced an SZ that has relatively finer and equiaxed grains due to dynamic recrystallization. Such microstructure development is strongly related to the dual action of induced-friction heat and severe plastic deformation by stirring. In addition, the microstructure of the TMAZ indicated the severity of the deformation, as illustrated by the elongation of grains in the flow direction near to the TMAZ/BM interface without the occurrence of dynamic recrystallization. In addition, the microstructures in the three zones contain a large amount of intermetallic particles dispersed into the aluminum matrix. Based on particle size analysis, most of the intermetallic particles are in the range of 1-3 μm, with minor differences in their distribution among the three regions.  Figure 3 shows optical micrographs illustrating the microstructure of each zone in the FSP plate. The structure of BM shows a typical deformed structure developed by rolling. The deformed structure is shown to be a lamellar type and aligned with the rolling direction. Most of the grains in the BM are small, with an average size of less than 10 µm. It is also evident that FSP produced an SZ that has relatively finer and equiaxed grains due to dynamic recrystallization. Such microstructure development is strongly related to the dual action of induced-friction heat and severe plastic deformation by stirring. In addition, the microstructure of the TMAZ indicated the severity of the deformation, as illustrated by the elongation of grains in the flow direction near to the TMAZ/BM interface without the occurrence of dynamic recrystallization. In addition, the microstructures in the three zones contain a large amount of intermetallic particles dispersed into the aluminum matrix. Based on particle size analysis, most of the intermetallic particles are in the range of 1-3 µm, with minor differences in their distribution among the three regions.  Furthermore, Figure 4 shows EBSD grain boundary reconstruction maps and corresponding Euler maps of the FSP sample. Low-angle grain boundaries (LAGBs) and high-angle grain boundaries (HAGBs) are shown as light grey and black lines, respectively. LAGBs present grain boundaries with a misorientation angle θ ≤ 15°, while HAGBs describe those with a misorientation angle θ ≥ 15°. Figure 4a shows the microstructure of the BM, indicating a large formation of fine grains with HAGBs. The corresponding Euler map in Figure 4b also shows the development of a lamellar structure. The microstructure of the SZ shown in Figure 4c indicates a relative reduction in the grain size due to the occurrence of dynamic recovery during FSP. The formation of recrystallized grains resulted in an increase in the fraction of HAGBs and the formation of grains of new orientations, as illustrated by the Euler map ( Figure 4d). Yet, the SZ still contains a large fraction of LAGBs (~50%), which suggests that the microstructure had partly undergone dynamic recrystallization during FSP. This resulted in heterogeneous microstructural development in the SZ having primarily two microstructural constituents: small dynamically recrystallized grains that are  Furthermore, Figure 4 shows EBSD grain boundary reconstruction maps and corresponding Euler maps of the FSP sample. Low-angle grain boundaries (LAGBs) and high-angle grain boundaries (HAGBs) are shown as light grey and black lines, respectively. LAGBs present grain boundaries with a misorientation angle θ ≤ 15 • , while HAGBs describe those with a misorientation angle θ ≥ 15 • . Figure 4a shows the microstructure of the BM, indicating a large formation of fine grains with HAGBs. The corresponding Euler map in Figure 4b also shows the development of a lamellar structure. The microstructure of the SZ shown in Figure 4c indicates a relative reduction in the grain size due to the occurrence of dynamic recovery during FSP. The formation of recrystallized grains resulted in an increase in the fraction of HAGBs and the formation of grains of new orientations, as illustrated by the Euler map ( Figure 4d). Yet, the SZ still contains a large fraction of LAGBs (~50%), which suggests that the microstructure had partly undergone dynamic recrystallization during FSP. This resulted in heterogeneous microstructural development in the SZ having primarily two microstructural constituents: small dynamically recrystallized grains that are dislocation-free, and larger recrystallized grains with a moderate dislocation density. The microstructure of TMAZ is shown in Figure 4e.

Friction Stir Processing
As discussed, many of the grains are heavily distorted due to the stirring action near the undeformed BM. This led to the breakage of HAGBs and thus a reduction in the fraction of HAGBs. The Euler map in Figure 4f also shows that dynamic recovery was limited in TMAZ since the amount of heat is expected to be lower than that produced in the SZ. In addition, Table 1 summarizes EBSD statistics for the average grain size and grain boundary misorientation. The results show that SZ consists of a relatively smaller grain size (6.5 µm), compared to the TMAZ (7.2 µm) and BM (8.2 µm). It is also shown that SZ has the maximum percentage of HAGBs (50.4%) compared to TMAZ (26.8%) and BM (32.9%), confirming the occurrence of dynamic recrystallization. On the other hand, the reduction of HAGBs in TMAZ also suggests that the structure development in TMAZ was solely controlled by the severe plastic deformation and the occurrence of dynamic recrystallization was very limited. This resulted in an increase in the formation of LAGBs, mostly shown as subgrain walls, and the breakage of grain boundaries of high-angle misorientations. dislocation-free, and larger recrystallized grains with a moderate dislocation density. The microstructure of TMAZ is shown in Figure 4e. As discussed, many of the grains are heavily distorted due to the stirring action near the undeformed BM. This led to the breakage of HAGBs and thus a reduction in the fraction of HAGBs. The Euler map in Figure 4f also shows that dynamic recovery was limited in TMAZ since the amount of heat is expected to be lower than that produced in the SZ. In addition, Table 1 summarizes EBSD statistics for the average grain size and grain boundary misorientation. The results show that SZ consists of a relatively smaller grain size (6.5 μm), compared to the TMAZ (7.2 μm) and BM (8.2 μm). It is also shown that SZ has the maximum percentage of HAGBs (50.4%) compared to TMAZ (26.8%) and BM (32.9%), confirming the occurrence of dynamic recrystallization. On the other hand, the reduction of HAGBs in TMAZ also suggests that the structure development in TMAZ was solely controlled by the severe plastic deformation and the occurrence of dynamic recrystallization was very limited. This resulted in an increase in the formation of LAGBs, mostly shown as subgrain walls, and the breakage of grain boundaries of highangle misorientations.    Moreover, the EBSD results demonstrate the formation of small equiaxed grains with HAGBs in SZ due to dynamic recrystallization during FSP. It is anticipated that limited growth of the newly formed grains will occur during post-dynamic recrystallization, i.e., metadynamic recrystallization. This is attributed to the presence of precipitates and intermetallic particles that can delay both static and dynamic recrystallization, including metadynamic recrystallization [18]. The development of different microstructure constituents in the SZ is expected to result in different static restoration behavior upon applying post heat treatment. Sakai et al. [19] have identified different restoration mechanisms during post annealing of hot-deformed metallic alloys. The small recrystallized nuclei, formed during hot deformation, may continue to grow during the early stages of post deformation annealing by the mechanism of metadynamic recrystallization. For the large recrystallized grains, the restoration process depends on the density of dislocation contained in the structure. If the dislocation density is low, below a critical density value required for recrystallization, then recovery occurs. For a higher dislocation density, the large grains may subsequently recrystallize statically.
In addition, the formation of recrystallized grains in SZ might also be affected by the presence of large second-phase particles. In such cases, recrystallization can be triggered by particle stimulated nucleation (PSN) for metallic alloys containing second-phase particles, such as in the case of AA6082 [20]. During plastic deformation, hard particles are expected to deform much less than the matrix phase. This typically leads to the development of strain gradient and lattice rotation around the particles, creating the so-called particle deformation zone (PDZ). In the case of the recrystallization of the deformed structure, the PDZ can act as a site for the nucleation of new grains via PSN. The size of particles for PSN is typically larger than 1 µm [20]. This is required to form an appreciable PDZ around the particle during the deformation. However, PSN is mainly effective for low-temperature deformation and it becomes less viable, but possible, for hot deformation processes such as FSP. The current findings show no strong correlation between the presence of second-phase particles and the development of fine grains in SZ during dynamic recrystallization. Also, it should be noted that second phase particles can have a dual effect on recrystallization since they can promote and hinder recrystallization. In the case of closely-spaced and small particles, recrystallization can be retarded since the particles can prevent subgrain and grain boundary movement by Zener pinning [21].

Artifical Aging
The effect of artificial aging on the microstructural development in the SZ of FSP AA6082 samples was examined using EBSD. To do that, three aging temperatures of 150 • C, 175 • C, and 200 • C were used for an aging period of 1 h, 6 h, and 12 h. Figure 5 shows EBSD grain boundary construction and Euler maps of the SZ for FSP samples aged at 150 • C. Aging at 1 h produced no significant difference in the grain size compared to those produced by the FSP condition ( Figure 5a). Also, the distribution of Euler orientations shown in Figure 5b is similar to the FSP condition. However, there is an increase in the LAGBs compared to the FSP sample. This is mostly likely attributed to the presence of a large number of subgrains of LAGBs. The results also show the scattered formation of fine grains with a size of less than 1 µm. Most of the fine grains possess HAGBs. Moreover, grain growth in some regions is shown to occur when aging at 150 • C for 6 h. This resulted in a reduction in the fraction of HAGBs, as demonstrated in Figure 5c,d. Subgrains of LAGBs are clearly shown to form within the large grains. The difference in microstructural development is strongly related to the variation in the dislocation density formed in the dynamically recrystallized structure during FSP. For grains with a low dislocation density, recovery is most likely to occur during post aging [19]. For grains with a high dislocation density, the grains may recrystallize statically after aging and subsequently grow. This indicates that both recovery and recrystallization had occurred during aging due to the microstructural inhomogeneity in the SZ induced by FSP. This is expected for recovery and recrystallization to occur since they have the same driving force, i.e., reduction in stored energy by a decrease in the amount of crystal defects. In addition, the results show the presence of small grains of a size of less than 1 µm, which are randomly nucleated in the large grains and at grain boundaries. When increasing the aging time to 12 h, recrystallization was shown to occur, as presented by the formation of fine recrystallized grains of HAGBs. The size of the fine grains is in the range of 1-3 µm. The distribution of fine grains in the structure generally takes the form of a necklace, as demonstrated in Figure 5e,f. Also, some regions had not gone through recrystallization as they contain subgrains of LAGBs. statically after aging and subsequently grow. This indicates that both recovery and recrystallization had occurred during aging due to the microstructural inhomogeneity in the SZ induced by FSP. This is expected for recovery and recrystallization to occur since they have the same driving force, i.e., reduction in stored energy by a decrease in the amount of crystal defects. In addition, the results show the presence of small grains of a size of less than 1 μm, which are randomly nucleated in the large grains and at grain boundaries. When increasing the aging time to 12 h, recrystallization was shown to occur, as presented by the formation of fine recrystallized grains of HAGBs. The size of the fine grains is in the range of 1-3 μm. The distribution of fine grains in the structure generally takes the form of a necklace, as demonstrated in Figure 5e,f. Also, some regions had not gone through recrystallization as they contain subgrains of LAGBs.     Figure 6 presents the EBSD grain boundary construction and Euler maps of the SZ for artificially aged samples at 175 • C. Aging for 1 h is shown to result in recrystallization and the formation of fine grains. This is similar to microstructure development observed for the sample aged at 150 • C for 12 h. Yet, the average grain size at 175 • C for 1 h is smaller than that obtained by aging at 150 • C for 12 h. This suggests that grain coarsening at 175 • C was limited due to precipitate formation that resulted in hindering grain boundary migration by Zener pinning. It can also be noticed that some large grains were not fully recrystallized. These large grains contain a mixture of subgrains of LAGBs and newly recrystallized fine grains of HAGBs. Increasing the aging time to 6 h resulted in relatively coarser grains and a higher fraction of HAGBs. A further increase in aging time to 12 h led to insignificant change in the restoration process, as demonstrated by the recovery of a deformed structure possessing LAGBs and the recrystallization of fine grains of HAGBs. grains. This is similar to microstructure development observed for the sample aged at 150 °C for 12 h. Yet, the average grain size at 175 °C for 1 h is smaller than that obtained by aging at 150 °C for 12 h. This suggests that grain coarsening at 175 °C was limited due to precipitate formation that resulted in hindering grain boundary migration by Zener pinning. It can also be noticed that some large grains were not fully recrystallized. These large grains contain a mixture of subgrains of LAGBs and newly recrystallized fine grains of HAGBs. Increasing the aging time to 6 h resulted in relatively coarser grains and a higher fraction of HAGBs. A further increase in aging time to 12 h led to insignificant change in the restoration process, as demonstrated by the recovery of a deformed structure possessing LAGBs and the recrystallization of fine grains of HAGBs.    Figure 7 shows the EBSD results of the SZ for artificially aged samples at 200 • C. Aging for 1 h produced a microstructure that is composed of fine recrystallized grains with HAGBs and large grains with subgrains of LAGBs. Compared to 175 • C aging, the formation of fine recrystallized grains is shown to occur, but to a lesser extent. At 6 h, the size of the recrystallized grains becomes coarser.
Many of the LAGBs that belong to subgrains changed into HAGBs, suggesting the formation of new recrystallized grains. Increasing the aging time to 12 h only caused limited grain coarsening of the recrystallized grains. Otherwise, the microstructure looks similar to that obtained by aging at 200 • C for 6 h. The large difference in Euler orientations for samples aged for 6 h and 12 h, presented in Figure 7d,f, confirms the strong occurrence of recrystallization.  Figure 7d,f, confirms the strong occurrence of recrystallization.  Table 2 summarizes the EBSD statistics for the average grain size, percentage of LAGBs, and HAGBs for each aging temperature and period. The results show that at 150 °C , the grain size reduces significantly from 5.5 μm at 1 h to 4.7 μm at 6 h and to 4.1 μm at 12 h. As described earlier, the formation of fine recrystallized grains with increasing aging time strongly contributed to grain size reduction. Also, the occurrence of recrystallization led to an increase in the percentage of HAGBs for the sample aged for 12 h (55.5%) after it was at its minimum (46.6%) at 6 h. In the case of aging at 175   Table 2 summarizes the EBSD statistics for the average grain size, percentage of LAGBs, and HAGBs for each aging temperature and period. The results show that at 150 • C, the grain size reduces significantly from 5.5 µm at 1 h to 4.7 µm at 6 h and to 4.1 µm at 12 h. As described earlier, the formation of fine recrystallized grains with increasing aging time strongly contributed to grain size reduction. Also, the occurrence of recrystallization led to an increase in the percentage of HAGBs for the sample aged for 12 h (55.5%) after it was at its minimum (46.6%) at 6 h. In the case of aging at 175 • C, recrystallization of fine grains occurred at a short aging period of 1 h that resulted in an average grain size of 3.55 µm. Limited grain growth occurred at 6 h and 12 h, resulting in an increase in grain size to 4.5 and 4.6 µm, respectively. The increase in aging time also resulted in an increase in HAGBs, suggesting that further recrystallization occurred for a long period of aging at 175 • C. As previously described, aging at 200 • C for 1 h provided less formation of fine grains of HAGBs. This resulted in a larger grain size (~6 µm) and lower fraction of HAGBs (40%) compared to aging at 175 • C for 1 h. The structure for the sample aged at 200 • C for 6 h became fully recrystallized and thus resulted in equiaxed grains with an average grain size of 5.3 µm, providing the maximum percentage of HAGBs of 66.4%. Additional aging to 12 h resulted in coarsening of the recrystallized grains. This led to an increase in the average grain size to 5.8 µm and a reduction in the HAGBs percentage to 58%. Figure 8 presents grain size histograms for the aged samples. In the case of sample aged at 150 • C for 1 h (Figure 8a), there is a relatively uniform grain size distribution from 1 to 10 µm, which looks similar to the distribution in the SZ for the FSP sample. Increasing the aging time to 6 h resulted in a higher frequency for grain size in the range of 1-4 µm, which suggests the growth of grain nuclei during aging and the development of subgrains with a higher misorientation angle (Figure 8b). Yet, some large grains are still present, with an average grain size of 15 µm. At 12 h of aging, recrystallization of fine grains occurred that resulted in an increase in the frequency of grains in the range of 1-4 µm (Figure 8c). °C , recrystallization of fine grains occurred at a short aging period of 1 h that resulted in an average grain size of 3.55 μm. Limited grain growth occurred at 6 h and 12 h, resulting in an increase in grain size to 4.5 and 4.6 μm, respectively. The increase in aging time also resulted in an increase in HAGBs, suggesting that further recrystallization occurred for a long period of aging at 175 °C . As previously described, aging at 200 °C for 1 h provided less formation of fine grains of HAGBs. This resulted in a larger grain size (~6 μm) and lower fraction of HAGBs (40%) compared to aging at 175 °C for 1 h. The structure for the sample aged at 200 °C for 6 h became fully recrystallized and thus resulted in equiaxed grains with an average grain size of 5.3 μm, providing the maximum percentage of HAGBs of 66.4%. Additional aging to 12 h resulted in coarsening of the recrystallized grains. This led to an increase in the average grain size to 5.8 μm and a reduction in the HAGBs percentage to 58%. Figure 8 presents grain size histograms for the aged samples. In the case of sample aged at 150 °C for 1 h (Figure 8a), there is a relatively uniform grain size distribution from 1 to 10 μm, which looks similar to the distribution in the SZ for the FSP sample. Increasing the aging time to 6 h resulted in a higher frequency for grain size in the range of 1-4 μm, which suggests the growth of grain nuclei during aging and the development of subgrains with a higher misorientation angle (Figure 8b). Yet, some large grains are still present, with an average grain size of 15 μm. At 12 h of aging, recrystallization of fine grains occurred that resulted in an increase in the frequency of grains in the range of 1-4 μm (Figure 8c).

Texture
The microstructure refinement by severe plastic deformation of FSP is greatly affected by the rotation of different parts of the original grains towards stable texture components. In the case of FSP, the stable texture components are strongly related to the predominant deformation mode of simple shear [22][23][24]. Shear textures are conventionally defined in terms of the crystallographic plane {hkl} and direction <uvw>, aligned with the shear plane and shear direction, respectively. In fcc metals, the shear textures are {h k l} <1 1 0> fiber and {1 1 1} <uvw> fiber. The main ideal orientations along these fibers are illustrated in Figure 9 by the (1 1 1) pole figure projected on the SD-SPN plane, where SD is the shear direction and SPN is the shear plane normal [25].

Texture
The microstructure refinement by severe plastic deformation of FSP is greatly affected by the rotation of different parts of the original grains towards stable texture components. In the case of FSP, the stable texture components are strongly related to the predominant deformation mode of simple shear [22][23][24]. Shear textures are conventionally defined in terms of the crystallographic plane {hkl} and direction <uvw>, aligned with the shear plane and shear direction, respectively. In fcc metals, the shear textures are {h k l} <1 1 0> fiber and {1 1 1} <uvw> fiber. The main ideal orientations along these fibers are illustrated in Figure 9 by the (1 1 1) pole figure projected on the SD-SPN plane, where SD is the shear direction and SPN is the shear plane normal [25].   Figure 10a shows the texture of BM, demonstrating a typical rolling texture of strong copper orientation for fcc metals. The texture at the SZ presented in Figure 10b mainly consists of B fiber of the simple shear texture, i.e. {hkl} <110>, depicted by green. This suggests that the plastic flow at the center of the SZ strongly arises from the shear stress along the pin surface, and thus the shear plane and shear direction are roughly parallel to the pin surface and the rotating direction of the tool, respectively [26]. The shear texture of the B fiber is also formed in TMAZ, as shown in Figure 10c, but clockwise rotated around the ND. Recrystallization texture of the Cube orientation, given in red, is also shown for TMAZ. Sato et al. [26] reported that regions relatively far from the SZ center do not display shear components similar to those detected at the center, but are rather affected by the shear stresses induced by the forward motion of the rotating pin and the rotation action of the tool shoulder. At these positions, the texture becomes a mixture of shear and recrystallization components. Figure 11 represents the texture development in SZ for aged samples. The results show that the shear deformation texture of the B fiber still existed, but rotated from the ideal shear axis and at a lesser intensity. This suggests that the grain formation of fine grains occurred in the SZ without large alteration of the SZ texture [27]. In addition, the aging treatments resulted in different recrystallization behaviors. In the case of 150 °C, the recrystallization texture of the Cube orientation was strongly revealed when increasing the aging time to 12 h. This is consistent with the formation B a se d on th e te x tu ra l d a ta g iv e n in Fig . 4 e,it m a y be d e d u ce d th a t th e sh e a r p la n e in o u r e x p e rim e n t w a s ro u g h ly p a ra lle l to th e T D -N D p la n e (i.e .,p in co lu m n su rfa ce ) a n d th a t th e sh e a r d ire ctio n w a s n e a rly a lo n g th e TD (i.e .,ta n g e n tia l to th e p in co lu m n su rfa ce ). T a k in g in to a cco u n t th a t th e m a te ria lin R e g io n 4 d ire ctly in te ra cte d w ith th e ro ta tin g p in d u rin g FS W ,th e d e v e lo p m e n t ofth is te x tu re a p p e a rs to be re a so n a b le .
It is n o te w o rth y th a t th e te x tu ra l p e a k s in th e e x p e rim e nta l p o le fi g u re a re slig h tly d e v ia te d fro m th e ir id e a l p o sitio n s (Fig s. 4e a n d 5 ). T h e o b se rv e d d iscre p a n cie s a re p ro b a b ly a sso -cia te d m a in ly w ith th e 3 • to o l tiltin g u se d in o u r e x p e rim e n t. O th e r p o ssib le re a so n s fo r th is e ffe ct in clu d e th e th re a d s on th e p in co lu m n su rfa ce (w h ich m a y ca u se so m e v a ria tio n in th e sh e a r p la n e /d ire ctio n ) a n d lim ite d sa m p lin g d u rin g E B S D m e a su re m e n ts.   Figure 10a shows the texture of BM, demonstrating a typical rolling texture of strong copper orientation for fcc metals. The texture at the SZ presented in Figure 10b mainly consists of B fiber of the simple shear texture, i.e. {hkl} <110>, depicted by green. This suggests that the plastic flow at the center of the SZ strongly arises from the shear stress along the pin surface, and thus the shear plane and shear direction are roughly parallel to the pin surface and the rotating direction of the tool, respectively [26]. The shear texture of the B fiber is also formed in TMAZ, as shown in Figure 10c, but clockwise rotated around the ND. Recrystallization texture of the Cube orientation, given in red, is also shown for TMAZ. Sato et al. [26] reported that regions relatively far from the SZ center do not display shear components similar to those detected at the center, but are rather affected by the shear stresses induced by the forward motion of the rotating pin and the rotation action of the tool shoulder. At these positions, the texture becomes a mixture of shear and recrystallization components. Figure 11 represents the texture development in SZ for aged samples. The results show that the shear deformation texture of the B fiber still existed, but rotated from the ideal shear axis and at a lesser intensity. This suggests that the grain formation of fine grains occurred in the SZ without large alteration of the SZ texture [27]. In addition, the aging treatments resulted in different recrystallization behaviors. In the case of 150 • C, the recrystallization texture of the Cube orientation was strongly revealed when increasing the aging time to 12 h. This is consistent with the formation of new recrystallized grains shown in Figure 5e. For samples aged at 175 • C, the Cube orientation is clearly presented after 1 h of aging and became weaker with increasing aging time. For both aging temperatures, the shear texture of the B fiber is partially preserved in the SZ, while the recrystallization texture of the Cube orientation is moderately formed. This suggests that the formation of hardening precipitates during aging was effective in hindering lattice rotation and limiting the grain growth of new crystallized grains. On the other hand, increasing the aging temperature to 200 • C resulted in an increase in the intensity of Cube orientation with aging time, while partially maintaining the shear texture. This indicates that recrystallization became strongly active by aging at 200 • C, thus promoting the growth of new recrystallized grains of Cube orientation. Also, it can be inferred that the precipitation during aging at 200 • C is not sufficiently effective for hindering grain growth and lattice rotation, as demonstrated for samples aged at 150 • C and 175 • C.   The effect of artificial aging on AA6082 samples processed by FSP has been further analyzed using XRD, as shown in Figure 12. In general, new intensities for the aluminum phase were shown to form after subjecting FSP samples to aging. Four distinct peak patterns of the Al matrix were clearly shown to form, corresponding to planes of (111), (200), (311) and (222), respectively. The only   The effect of artificial aging on AA6082 samples processed by FSP has been further analyzed using XRD, as shown in Figure 12. In general, new intensities for the aluminum phase were shown to form after subjecting FSP samples to aging. Four distinct peak patterns of the Al matrix were clearly shown to form, corresponding to planes of (111), (200), (311) and (222), respectively. The only The effect of artificial aging on AA6082 samples processed by FSP has been further analyzed using XRD, as shown in Figure 12. In general, new intensities for the aluminum phase were shown to form after subjecting FSP samples to aging. Four distinct peak patterns of the Al matrix were clearly shown to form, corresponding to planes of (111), (200), (311) and (222), respectively. The only exception is for the sample aged at 150 • C for 1 h, showing similar peak formation to that obtained in the FSP sample. It can also be generally seen that the (111) and (200) intensities become stronger with either increasing aging time or aging temperature, suggesting that the current aging treatments promoted recrystallization in the SZ with either increasing aging time or aging temperature. No specific intermetallic phases were identified and noted on their respective peaks. Generally, the absence of other peaks of alloying elements is mainly attributed to the limitation of X-ray in detecting phases with an amount of less than 2% volume fraction [28]. exception is for the sample aged at 150 °C for 1 h, showing similar peak formation to that obtained in the FSP sample. It can also be generally seen that the (111) and (200) intensities become stronger with either increasing aging time or aging temperature, suggesting that the current aging treatments promoted recrystallization in the SZ with either increasing aging time or aging temperature. No specific intermetallic phases were identified and noted on their respective peaks. Generally, the absence of other peaks of alloying elements is mainly attributed to the limitation of X-ray in detecting phases with an amount of less than 2% volume fraction [28].

Hardness
The Vickers microhardness profiles of the AA6082 sample in the FSP condition are shown in Figure 13. The indentations were made at the SZ area at three depths from the processed surface (0.5 mm, 1.5 mm, and 2.5 mm, respectively), and at the BM region. The microhardness of the BM was measured to be 92.5 Hv, and it is depicted as a horizontal line in the plot. FSP is shown to result in significant softening in the SZ, reducing the microhardness to 64 Hv on average. The reduction in hardness in SZ is due to dynamic recrystallization facilitated by the combined effect of plastic deformation and heat induced by friction during FSP. The microhardness reduction extended over a wide distance of approximately 12 mm from the center of the SZ. The measurements at 0.5 mm from the processed surface are shown to provide the highest hardness, while the lowest hardness occurred at the furthest line from the processed surface (2.5 mm). This indicated that the fastest cooling occurred at the processed surface, resulting in a finer grain size and enhanced reformation of the hardening precipitates. Moreover, it can be noticed that there is a variation in hardness values in the SZ and TMAZ. Such variation is due to the difference in the amount of local heat in the processed material occurring during the thermal cycle, which can remarkably affect the dissolution of the hardening precipitates during heating and later the precipitates reformation process upon cooling [27]. Also, the variation in hardness can be related to the newly redistributed locations of second phase particles and precipitates, and to the fragmentation of the precipitates due to intense plastic deformation [29].

Hardness
The Vickers microhardness profiles of the AA6082 sample in the FSP condition are shown in Figure 13. The indentations were made at the SZ area at three depths from the processed surface (0.5 mm, 1.5 mm, and 2.5 mm, respectively), and at the BM region. The microhardness of the BM was measured to be 92.5 Hv, and it is depicted as a horizontal line in the plot. FSP is shown to result in significant softening in the SZ, reducing the microhardness to 64 Hv on average. The reduction in hardness in SZ is due to dynamic recrystallization facilitated by the combined effect of plastic deformation and heat induced by friction during FSP. The microhardness reduction extended over a wide distance of approximately 12 mm from the center of the SZ. The measurements at 0.5 mm from the processed surface are shown to provide the highest hardness, while the lowest hardness occurred at the furthest line from the processed surface (2.5 mm). This indicated that the fastest cooling occurred at the processed surface, resulting in a finer grain size and enhanced reformation of the hardening precipitates. Moreover, it can be noticed that there is a variation in hardness values in the SZ and TMAZ. Such variation is due to the difference in the amount of local heat in the processed material occurring during the thermal cycle, which can remarkably affect the dissolution of the hardening precipitates during heating and later the precipitates reformation process upon cooling [27]. Also, the variation in hardness can be related to the newly redistributed locations of second phase particles and precipitates, and to the fragmentation of the precipitates due to intense plastic deformation [29]. The effect of hardening precipitates formed by aging on the microhardness evolution of FSP was also examined as presented in Figure 14. For samples aged at 150 °C for 1 h, the hardness at the SZ varied for each indentation line, with a hardness of 87 Hv, 74 Hv, and 64 Hv for lines 1, 2 and 3, respectively ( Figure 14a). Additionally, the hardness values overall were higher for line 1, which is 0.5 mm from the processed surface, compared to the readings from lines 2 and 3. Such differences indicate that precipitations occurred heterogeneously in the SZ, resulting in a stronger formation of hardening precipitates near to the top surface. The microhardness at TMAZ remains approximately unchanged, representing the lowest hardness values within the processed area. This is most likely attributed to the overaged microstructure resembled by the coarsening of the hardening precipitates in TMAZ that were previously subjected to heat during FSP [30]. A similar finding was also reported by Jamshidi Aval and Serajzadeh [16], who examined the post aging of AA6061 subjected to FSW and indicated low values of hardness in TMAZ/HAZ after natural aging for a long period of 250 days. Moreover, increasing the aging time to 6 h resulted in an increase in the hardness values at the SZ for all lines to 79-86 Hv, forming a similar hardness pattern to that shown in Figure14b. At 12 h of aging, the microhardness showed an additional increase in hardness to about 90 Hv, while TMAZ remained The effect of hardening precipitates formed by aging on the microhardness evolution of FSP was also examined as presented in Figure 14. For samples aged at 150 • C for 1 h, the hardness at the SZ varied for each indentation line, with a hardness of 87 Hv, 74 Hv, and 64 Hv for lines 1, 2 and 3, respectively ( Figure 14a). Additionally, the hardness values overall were higher for line 1, which is 0.5 mm from the processed surface, compared to the readings from lines 2 and 3. Such differences indicate that precipitations occurred heterogeneously in the SZ, resulting in a stronger formation of hardening precipitates near to the top surface. The microhardness at TMAZ remains approximately unchanged, representing the lowest hardness values within the processed area. This is most likely attributed to the overaged microstructure resembled by the coarsening of the hardening precipitates in TMAZ that were previously subjected to heat during FSP [30]. A similar finding was also reported by Jamshidi Aval and Serajzadeh [16], who examined the post aging of AA6061 subjected to FSW and indicated low values of hardness in TMAZ/HAZ after natural aging for a long period of 250 days. Moreover, increasing the aging time to 6 h resulted in an increase in the hardness values at the SZ for all lines to 79-86 Hv, forming a similar hardness pattern to that shown in Figure 14b. At 12 h of aging, the microhardness showed an additional increase in hardness to about 90 Hv, while TMAZ remained at a low hardness of about 65 Hv. The SZ hardness values exceeded the hardness of the BM region subjected to a similar aging condition (82 Hv). The drop of the BM hardness is mainly attributed to the prolonged aging period that resulted in coarsening of the hardening precipitates. Also, it has been noticed in Figure 14c that the prolonged aging of 12 h resulted in a sudden drop in the hardness in a few SZ points that are close to TMAZ. Such a drop indicates that the development of hardening precipitates occurred inhomogeneously, resulting in localized coarsening of the precipitates, and this contributed to the sudden drop in the hardness. Figure 14d-f presents the hardness profile for aged samples at 175 • C. For 1 h of aging, the hardness profile is similar to that obtained by 150 • C with a similar aging time. In particular, the hardness values in SZ range between 69 and 72 Hv, which are below the BM value of 88.7 Hv. Upon aging for 6 h, the hardness changed significantly at the SZ, with a maximum value reaching 90 Hv. The hardness at the TMAZ also gradually increased to about 70 Hv. For 12 h, it can be clearly seen that the hardness at the SZ has settled to the highest values between 90 and 93 Hv, which are above the BM hardness (86 Hv), while the TMAZ hardness slightly increased to 73 Hv. Unlike aging at 150 • C, a sudden drop in the SZ hardness was not observed in samples aged at 175 • C. This indicates the uniformity of hardness evolution within the SZ. Moreover, Figure 14g-i indicate that aging at 200 • C resulted in different hardness development when compared to that shown for aging treatments at 150 • C and 175 • C. At 1 h, the SZ hardness showed a remarkable increase to 78 Hv compared to the sample in the FSP condition (64 Hv). The hardness in TMAZ is low, at about 60 Hv, while the BM showed a drop from 92.5 Hv in the as-received condition ( Figure 13) to about 84 Hv (Figure 14g). After 6 h of aging, there is a noticeable reduction in the SZ hardness to approximately 68 Hv, while the BM hardness gradually dropped to about 75 Hv. Increasing aging time to 12 h resulted in an additional reduction in the hardness for both SZ and BM, as they became approximately identical (70 Hv). Due to the use of a high aging temperature of 200 • C, the hardness profiles suggest that the processed aluminum samples reached a stage of overaging, thereby decreasing the alloy strength to a minimum of 70 Hv for both SZ and BM. It can also be noticed that a sudden drop in the hardness occurred in the SZ during 200 • C aging. This supports the previous findings presented in Figure 14c, which suggest that localized softening occurred due to different rates of precipitate formation and subsequent coarsening. Table 3 summarizes the average hardness values in the SZ and BM for FSP and aged AA6082 samples. It is observed that the average hardness in the SZ increases with increasing aging time to about 90 Hv. In the case of aging at 150 • C and 175 • C, the hardness evolution of BM looks similar, but higher hardness values are obtained for 175 • C at 12 h. This generally indicates that aging at 175 • C provided the optimum strengthening effect for both processed area and BM. In contrast, aging at 200 • C only resulted in a hardness increase for a short aging period of 1 h. Increasing aging time resulted in a significant hardness reduction for both processed area and BM, suggesting the occurrence of overaging at this relatively high aging temperature. The use of post weld heat treatment (PWHT) on FSP/FSW of 6000 series aluminum alloys has been previously investigated. Sato et al. [30] used PWHT for friction stir welded AA6063 at 175 • C for 5 h and 12 h and indicated a recovery of the hardness values in the SZ to that of BM; only partial recovery to hardness occurred in TMAZ. The increase in hardness was attributed to the reprecipitation of a large density of needle-shaped precipitates β" in the SZ since there was an abundance of solute atoms of magnesium and silicon. In TMAZ, a high density of β precipitates formed, consuming a large quantity of solutes, and thereby it was very difficult to form the needle-shaped precipitates β". Also, Cabibbo et al. [14] have examined the PWHT of FSW of AA6056 and showed a considerable increase in strength of the joint due to the formation of a high density of fine Mg 2 Si precipitates. In addition, El-Danaf and El-Rayes [15] examined the effect of PWHT on FSW of AA6082 at 175 • C for 5 h and 12 h. Only partial recovery in the hardness of the joint occurred due to the re-precipitation of hard β" particles during PWHT. There was no significant increase in the grains size after PWHT, suggesting that the re-precipitation of the β" restricted any grain growth. Mg2Si precipitates. In addition, El-Danaf and El-Rayes [15] examined the effect of PWHT on FSW of AA6082 at 175 °C for 5 h and 12 h. Only partial recovery in the hardness of the joint occurred due to the re-precipitation of hard β″ particles during PWHT. There was no significant increase in the grains size after PWHT, suggesting that the re-precipitation of the β″ restricted any grain growth. The effect of aging on hardness development has also been examined in Al-Mg-Si alloys subjected to severe plastic deformation. Cerri and Leo [31] examined the artificial aging of AA6082 subjected to equal-channel angular pressing (ECAP) and reported that the use of high aging temperatures resulted in an increasing softening with time due to recovery and grain coarsening. At lower aging temperatures, the hardness remained almost constant owing to enhanced precipitation hardening over recovery and grain coarsening. Faré et al. [32] also studied the aging behavior of the 6082 alloy processed by ECAP and asymmetric rolling. It was indicated that aging at 180 °C led to a fast aging process, resulting in a continuous drop in hardness with increasing time due to the overwhelming effects of structure restoration. On the contrary, aging at 130 °C provided a strong precipitate hardening effect in the ultrafine-grained material. In addition, other studies examined the effect of post annealing on precipitation and microstructural evolution in AA6082 subjected to severe rolling reductions [33,34]. It was reported that at a low annealing temperature of 150 °C, the formation of new subgrains occurred with an increase in the faction of HAGBs. At higher annealing The effect of aging on hardness development has also been examined in Al-Mg-Si alloys subjected to severe plastic deformation. Cerri and Leo [31] examined the artificial aging of AA6082 subjected to equal-channel angular pressing (ECAP) and reported that the use of high aging temperatures resulted in an increasing softening with time due to recovery and grain coarsening. At lower aging temperatures, the hardness remained almost constant owing to enhanced precipitation hardening over recovery and grain coarsening. Faré et al. [32] also studied the aging behavior of the 6082 alloy processed by ECAP and asymmetric rolling. It was indicated that aging at 180 • C led to a fast aging process, resulting in a continuous drop in hardness with increasing time due to the overwhelming effects of structure restoration. On the contrary, aging at 130 • C provided a strong precipitate hardening effect in the ultrafine-grained material. In addition, other studies examined the effect of post annealing on precipitation and microstructural evolution in AA6082 subjected to severe rolling reductions [33,34]. It was reported that at a low annealing temperature of 150 • C, the formation of new subgrains occurred with an increase in the faction of HAGBs. At higher annealing temperatures, subgrain growth and recrystallization took place. Also, post annealing was shown to cause an increase in hardness due to the formation of second-phase precipitates, with a maximum hardness for samples treated at 160 • C for 14 h. Additional aging times resulted in a drop in the hardness due the post dynamic recovery and substructure coarsening. Furthermore, Chrominski [35] examined the aging behavior of AA6082 subjected to hydrostatic extrusion and pointed out that at short times of aging, precipitation hardening had a great influence on the increase of hardness rather than softening by dislocation annihilation or grain growth. After 14 h of aging, precipitation was shown to remain almost unchanged, but the hardness decreased due to grain growth and recovery processes.

Conclusions
Artificial aging was applied on aluminum alloy AA6082 initially subjected to FSP. The main objective was to evaluate the effect of artificial aging on the microstructure, texture, and mechanical properties of the processed area. This was achieved by using different aging temperatures and aging times (150 • C, 175 • C, and 200 • C and for 1 h, 6 h and 12 h). The following conclusions can be drawn: • FSP resulted in the formation of fine and equiaxed grains with predominant HAGBs in the SZ due to the occurrence of dynamic recrystallization. The FSP produced grain refinement in the SZ to 6.5 µm, as compared to the BM and TMAZ (8.2 and 7.2 µm, respectively). A high fraction of HAGBs was recorded in the SZ, confirming the formation of recrystallized grains in the SZ. • Long aging periods and/or high aging temperatures caused recovery, followed by recrystallization of fine grains in the range of 1-3 µm within the SZ. Recovery occurred for short aging periods at 150 • C, while the formation of fine recrystallized grains was shown after aging for 12 h. Aging at 175 • C resulted in the recrystallization of fine grains upon aging for 1 h, while simultaneously increasing the fraction of HAGBs when increasing the aging period to 6 and 12 h. In the case of 200 • C aging, a reduction of grain size initially occurred at 1 h of aging due to recrystallization. Longer aging times resulted in grain coarsening to 6 µm and thereby lowering the fraction of HAGBs. • FSP predominantly provided a simple shear texture in the SZ with a main component of B fiber. Increasing aging temperature and/or aging time was shown to weaken the B fiber and resulted in the formation of the recrystallization texture of Cube orientation. The formation of new fine grains and subsequent grain growth was particularly essential for strengthening the Cube orientation by the aging treatments used in the current study. • Applying FSP resulted in significant softening in the SZ (64 Hv) compared to the BM (92.5 Hv). This is mostly attributed to the dissolution of the hardening precipitates β" by the excessive heat of FSP. Aging at 175 • C for 12 h provided maximum recovery of the hardness in the SZ (90 Hv), while maintaining the initial hardness value of the BM without a significant reduction (86 Hv). Aging at 150 • C also enhanced the hardness of the SZ after 12 h (90 Hv), but it lowered the hardness of BM (77 Hv). On the other hand, samples aged at 200 • C for 12 h showed a significant reduction in hardness for SZ (68.5 Hv) and BM (73 Hv), which implies the occurrence of overaging.