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Article

Analysis of Different Solution Treatments in the Transformation of β-AlFeSi Particles into α-(FeMn)Si and Their Influence on Different Ageing Treatments in Al–Mg–Si Alloys

by
Florentino Alvarez-Antolin
*,
Juan Asensio-Lozano
,
Alberto Cofiño-Villar
and
Alejandro Gonzalez-Pociño
Materials Pro Group, Department of Materials Science and Metallurgical Engineering, University of Oviedo, Independencia 13, 33004 Oviedo, Spain
*
Author to whom correspondence should be addressed.
Metals 2020, 10(5), 620; https://doi.org/10.3390/met10050620
Submission received: 7 April 2020 / Revised: 28 April 2020 / Accepted: 7 May 2020 / Published: 10 May 2020
(This article belongs to the Special Issue Casting and Solidification of Light Alloys)

Abstract

:
In the as-cast state, Al–Mg–Si alloys are not suitable for hot forming. They present low ductility due to the presence of intermetallic β-AlFeSi particles that form in the interdendritic regions during the solidification process. Homogenization treatments promote the transformation of these particles into α-(FeMn)Si particles, which are smaller in size and more rounded in shape, thus improving the ductility of the material. This paper analyses the influence of various solution treatments on the transformation of β-AlFeSi particles into α-(FeMn)Si particles in an Al 6063 alloy. Their effect on different ageing treatments in the 150–180 °C temperature range is also studied. An increase in the solution temperature favours greater transformation of the β-AlFeSi particles into α-(FeMn)Si, dissolving a greater amount of Si, thereby having a significant effect on subsequent ageing. We found that as the dwell time at a temperature of 600 °C increases, the rate of dissolution of the Fe atoms from α-(FeMn)Si particles exceeds the rate of incorporation of Mn atoms into said particles. This seems to produce a delay in reaching the peak hardness values in ageing treatments, which warrants further research to model this behaviour. The optimal solution treatment takes place at around 600 °C and the highest obtained peak hardness value is 104 HV after a 2 h solution treatment at said temperature and ageing at 160 °C for 12 h.

1. Introduction

Aluminium alloys usually have iron as a common impurity. The maximum equilibrium solubility of Fe in solid aluminium is very low. Thus, most Fe forms Fe-rich intermetallic compounds together with other elements, which appear as needles or sharp edges in the microstructure. Some types of Fe-rich intermetallic compounds are very harmful to mechanical properties, especially ductility [1]. The particles present in Al–Mg–Si alloys during solidification are mostly β-AlFeSi (generally the β-Al5FeSi phase), α-AlFeSi (generally the α-Al8Fe2Si phase) and Mg2Si [1,2,3]. These alloys are not suitable for hot forming processes in the as-cast state or in processes of intensive deformation, as occurs in extrusion. Their ductility is too low, mainly due to the presence of intermetallic β-AlFeSi particles that locate at interdendritic regions, giving rise to the occurrence both inside the α-Al grains and at their grain boundaries after solidification is completed [4]. These particles usually have an acicular morphology in the polished plane. Hot ductility is impaired by the presence of these particles, decreasing significantly as their content increases. The purpose of the high-temperature homogenization process is the chemical homogenization of the dendrites, as well as the simultaneous fragmentation of the β-Al5FeSi precipitates, thus avoiding their continuity along the grain boundaries and favouring their conversion into α-Al(FeMn)Si particles with rounded edges, which increase ductile behaviour. This conversion must be complete in hot extrusion processes, as they take place in a single stage with intensive deformation and in a very short time. Hot rolling processes that obtain flat rolled products and multi-pass hot strip mills enable the decrease in temperatures and homogenization times without completing the total transformation of β particles into α particles. β-AlFeSi particles can lead to local crack initiation and induce surface defects on the extruded material. The more rounded α-Al(FeMn)Si particles in the homogenized material improve the extrudability of the material as well as the surface quality of the extruded material [5]. The morphology of the Fe-rich phase is related to many factors, such as the composition of the alloy, the cooling rate, and the content of Fe. During solidification, for example, α-Al8Fe2Si tends to form at higher cooling rates than β-Al5FeSi [6]. The presence of Mn can change the morphology of the acicular Fe-rich phase and form a granular intermetallic α-Al(MnFe)Si phase [7,8]. The formation of the β-AlFeSi particles is prior to, or at least concurrent with, the solidification of the alloy, which is why these precipitates are found in the interdendritic regions. The same grain can eventually encompass several dendrites. Therefore, these particles can appear inside the grains. As a result, the above processes lead to an increase in hot ductility [9]. A homogenization heat treatment promotes the transformation of these needle-like particles into smaller particles with more rounded shapes denoted as α-(FeMn)Si, α-Al8(FeMn)2Si or α-Al12(FeMn)3Si [5], which allows an enhancement in the ductility of the material [9,10,11,12,13,14]. The main force inducing the transformation of the β particles into α particles is found in the difference of Fe concentration between the Al matrix and the β particles themselves. It has been found that an Fe content in the alloy between 0.15% and 0.25% favours the appearance of smaller volume fractions of β intermetallics during solidification and promotes fine acicular morphologies, favouring a faster β → α transformation [15]. Moreover, the Mn in turn modifies this inducing force by causing variations in the concentration of Fe in the matrix and β interfaces. Kuijpers et al. determined that the optimal rate of transformation of β particles into α particles occurs when the manganese concentration falls within the 0.02% to 0.2% range [16]. With an increase in solution time, the acicular morphology of the β-AlFeSi particles can be transformed into rounded shapes and the α-Al8(FeMn)2Si phase can be formed. A minimal amount of Mn is needed to promote this transformation. The desirable Mn/Fe ratio could be around 0.5. The α-(FeMn)Si particles present an Fe/Si atomic ratio that is higher than that of its homologous β phase. Therefore, the solid solution of Si in the matrix phase accordingly increases, favouring subsequent hardening via an ageing treatment [12,17]. Lui et al. concluded that the (Fe + Mn)/Si atomic ratio remains constant in homogenization treatments within the 550–580 °C temperature range [18]. In addition to the aforementioned objectives, the homogenization treatment also aims to reduce the microsegregation produced during non-equilibrium solidification and endow the material with a fine, homogeneous structure of precipitates that ensures its subsequent manufacture. The final mechanical properties are determined by the solution heat treatment, quench rate and ageing heat treatment employed. In the solution heat treatment, the aim is to dissolve the phases containing Mg and Si. The temperatures employed in these alloys usually fall within the 460–530 °C range [19]. Chen et al. placed the optimal treatment at 520 °C for 3.5 h [20]. The ageing of these alloys begins with the formation of clusters in the Guinier–Preston (GP) zones followed by sequential precipitation of the β” phase and other metastable phases until precipitation of the β equilibrium phase is achieved [21]. The high level of saturation and high concentration of voids that the α-Al phase presents after quenching promotes the rapid formation of Si clusters and/or GP zones. These clusters have a high concentration of solute and maintain absolute coherence with the matrix, although elastic stresses are induced around them due to the difference in size between the atoms of the solute and those of the solvent. At this point, there is an increase in hardness, as these clusters/zones constitute a major obstacle to the displacement of dislocations [22,23]. Transition precipitates that are coherent with the matrix may nucleate from these zones. The increase in strength is defined by the size of the precipitates, their distribution, and their coherence with the matrix. In these alloys, the precipitate responsible for hardening is the β” (associated with the Mg2Si phase) [22,23,24,25]. It was found that the width of the precipitate-free zones (PFZs) was significant and optimal precipitation was associated with low thickness [26,27]. The temperatures used in the solubilization treatment and the dwell times at these temperatures seem to have a significant influence on the strength obtained after the ageing treatment. An increase in the temperature or dwell times at the aforementioned temperatures seems to favour an increase in strength after ageing [19,28]. Nandy et al. managed to obtain a peak hardness value of 90 HV by ageing at 175 °C for around 8 h, after a solution treatment at 525 °C for 2 h [29]. Yuksel obtained a maximum hardness value of nearly 100 HV by means of a solution treatment at 535 °C for 2 h and ageing at 204 °C for 2 h [25]. Note that the greatest decrease in hardness due to over-ageing was obtained at this same temperature compared to lower ageing temperatures. Several authors concluded that the rate of cooling prior to ageing and after the solubilization treatment seems to influence the peak hardness value after the ageing treatment. This cooling rate should be as high as possible in order to achieve the maximum supersaturation of Si and Mg in solid solution [24,30,31,32]. The most sensitive temperature range at industrial cooling rates seems to be between 450 and 250 °C [24,31,33]. Prolonged solubilization treatments are necessary in order to ensure the total dissolution of the Mg2Si formed in the cooling after chemical homogenization. As a form of validation, it is likewise necessary to employ a cooling rate which is fast enough to avoid the premature precipitation of Mg2Si. This would allow the full potential of structural hardening to be available in the subsequent ageing process.
The aim of this paper is to analyse the influence of various solution treatments, employing quenching in water, on the transformation of the β-AlFeSi particles in an Al 6063 alloy into α-(FeMn)Si particles and their possible influence on different ageing treatments carried out in the 150–180 °C range.

2. Materials and Methods

One hundred twenty specimens were taken from the intermediate zone of the radius of a number of 200-mm-diameter slabs in the as-cast state. Table 1 shows the chemical composition of the as-cast material. These slabs were manufactured by continuous casting in discontinuous processes, with cooling and lubrication by demineralized water in the die. The round aluminium products had an approximate diameter of 228 mm and a length of 12 m. The cooling rates measured at the centre of these products were 1 K/s, and 20 K/s at the surface. The specimens had a cubic geometry measuring 12–15 mm per side. One hundred sixteen of these specimens were subjected to four solution treatments, employing three different ageing temperatures for each. Quenching in water at 15 °C was used after the solution treatments. Figure 1 outlines the experimental work carried out. The 120 specimens were distributed as follows:
(1)
108 specimens were used to obtain the hardness profiles: 4 different solution treatments were carried out, employing 3 ageing treatments per solution treatment, with a total of 9 specimens in each ageing treatment.
(2)
8 specimens had no ageing. There were 2 specimens after each solution treatment, one was used for metallographic inspection and calculation of the material’s hardness, while the other was used for differential scanning calorimetry (DSC).
(3)
The remaining 4 specimens were analysed in the as-cast state.
Metallographic inspection was carried out using an optical microscope and a scanning electron microscope.
Preparation of the metallographic specimens was carried out by cutting with a SiC disc, cold mounting with an epoxy resin, grinding with SiC paper of different abrasive grain sizes ranging from grit 240 to 600 then finally polishing in three steps with textile cloths using different types of abrasives in each step. In the first step, 6 and 1 µm diamond paste was used, while a 0.5 µm alumina solution in distilled water was used in the second step. In the third stage, a 0.05 µm colloidal silica solution, which was also in distilled water, was utilized.
The etching reagents used in the optical microscopy analysis were:
(1)
2 mL HF, 3 mL HCl, 5 mL HNO3 and 190 mL distilled water.
(2)
A solution made of 4 g KMnO4, 1 g NaOH and 100 mL distilled water. This reagent reveals the chemical heterogeneities derived from dendritic microsegregation.
The optical microscope used was a NIKON Epiphot 200 (Nikon, Tokyo, Japan) and the images were obtained using Beuhler Omnimet Enterprise image analyser software (5.0, Beuhler, Lake Bluff, USA). The scanning electron microscope employed was a JEOL JSM-5600 (JEOL, Nieuw-Vennep, The Netherlands). The Fe/Si atomic ratio in the α-Al(FeMn)Si particles was determined on metallographic samples in the polished state, without etching with a chemical reagent. Energy dispersive X-ray (EDX) microanalysis was used for this purpose, randomly analysing 30 particles per specimen (20 kV with reflections of up to 10 keV).
Vickers hardness values were obtained under the application of a 300 N load. The results correspond to the mean value obtained from 12 indentations per specimen.
The differential scanning calorimeter used was a Mettler Toledo DSC 822e (Metter Toledo, Schwerzenbach, Switzerland). The heating rate was 10 °C/min, and the test was conducted between 25 and 500 °C. The results obtained by DSC will not provide us with the isothermal temperature at which the precipitation of the metastable phases that cause structural hardening takes place. During the DSC test, these temperatures are obtained by means of a heating ramp and are therefore always higher than the temperatures used isothermally for artificial ageing. However, when the aim is to compare various ageing treatments, this test allows us to compare whether said precipitation of structural hardening will occur sooner or later.

3. Results

Figure 2 shows the microstructure obtained in the as-cast state. It can be seen that the microstructure presents dendritic segregation and precipitation of β-Al5FeSi particles in the segregated zones, preferably at the grain boundaries. Figure 3 shows images of this microstructure obtained using electron channelling contrast imaging (ECCI) [34]. The elongated, acicular morphology of the β-Al5FeSi particles can be observed, forming a more or less continuous network through the grain boundaries network of the α-Al phase. It can also be seen that the grain size is around 200–250 μm. Figure 4 shows the microstructure obtained following the solution treatments with cooling in water. A homogenized microstructure can be seen in all cases, with no dendritic segregation. A decrease in the volume fraction of AlFeSi particles and loss of their continuity were likewise observed. Figure 5 shows the transformation of the microstructure during the homogenization treatment. Figure 5a shows the microstructure obtained in the as-cast state. The β-Al5FeSi particles and the Mg2Si phase can be observed, both located at a grain boundary. Figure 5b shows the microstructure after solubilization at 600 °C, employing cooling in water. This treatment also allows the solubilization of the Mg2Si phase and the transformation of the β-Al5FeSi particles into α-Al8(FeMn)2Si particles. Cooling in water prevented solid-state precipitation of Mg2Si.
Figure 6 shows the Fe/Si atomic ratio and the atomic percentage of Mn in the α-Al(FeMn)Si particles, while Figure 7 shows the (Fe + Mn)/Si ratio, along with the atomic percentages of Si and Fe. It can be observed that the Fe/Si ratio was higher in treatments at 600 °C than in treatments at 550 °C, a finding that could be justified by the greater dissolution of Si atoms at 600 °C. This would allow an increase in the potential for structural hardening. However, this ratio decreased when the duration of the treatment was 4 h. Note that the atomic % of Fe in the α particles was much lower in the treatments at 600 °C, being lower with dwell times of 4 h versus 2 h. Moreover, the β-AlFeSi particles in the as-cast state do not contain Mn atoms. However, as the dwell times of the treatment temperature increased, the atomic content of Mn in the α-Al(FeMn)Si particles also increased.
The hardness value in the as-cast state was 40 HV and the hardness value obtained after these treatments was 45 HV, with no differences in hardness being found between the different solution treatments. The hardness test was carried out immediately after these treatments.
Figure 8 shows the results obtained after the DSC analysis. Two main exothermic peaks were detected, designated as A and C. Peak A corresponds to precipitation of the β”and β’ phases. In between peaks A and C is the endothermic peak B that corresponds to the dissolution of these phases. Lastly, peak C corresponds to the precipitation of the β phase [35,36,37,38,39,40,41,42]. The endothermic peak prior to the exothermic peak A shows the dissolution of the GP zones formed during natural ageing. The results of the DSC test provide the temperatures at which the structural hardening precipitations are verifiable when this temperature is reached by means of a heating ramp. In our case, the heating rate is 10 °C/ min. This means that these temperatures cannot be compared with the isothermal ageing temperatures, the latter being necessarily lower. However, when the aim is to compare various ageing treatments, this test allows us to compare whether the structural hardening will occur sooner or later. The solution treatment at 600 °C with a dwell time of 4 h produced the greatest delay in the formation of the metastable transition phases (Peak A) and their subsequent dissolution (Peak B). This delay could be related to the dissolution of the Fe atoms that were observed in the previous solution treatment at this temperature with prolonged dwell times, which could be grounds for further investigation in this regard.
Figure 9 shows the hardness profiles obtained after the ageing treatments. The peak hardness values were obtained with solution treatments at 600 °C, which are the ones that dissolved the highest % Si from the β-AlFeSi particles. This would allow more Si to be available in solid solution for the subsequent precipitation of the metastable β” phase during ageing. The peak hardness value was 104 HV after the solution treatment at 600 °C for 2 h and ageing at 160 °C for 12 h. Very similar hardness profiles following the solution treatment at 550 °C were obtained with dwell times of 2 and 4 h. However, the peak hardness values obtained after a dwell time of 4 h at 600 °C were delayed in the three ageing temperatures compared to the 2 h dwell time. This fact may be conditioned by the dissolution of Fe atoms observed after the 4 h dwell time at 600 °C.

4. Conclusions

This paper analyses the influence of solution treatments on the transformation of β-AlFeSi particles into α-(FeMn)Si particles and their possible influence on different ageing treatments carried out in the 150–180 °C range. The main conclusions are:
(1)
The Fe/Si atomic ratio increased with increasing solution treatment temperature from 550 to 600 °C. This reflects a greater degree of transformation of β-Al5FeSi particles into α-Al8(FeMn)2Si particles, and a greater potential for structural hardening.
(2)
In the transformation of β-Al5FeSi particles into α-Al8(FeMn)2Si, a greater dissolution of both Si and Fe atoms was observed in the matrix when the solution treatment was carried out at 600 °C. The dissolution of Fe was somewhat more pronounced when the dwell times were increased from 2 to 4 h.
(3)
At a solution temperature of 550 °C, the (Fe + Mn)/Si atomic ratio remained practically constant. However, at 600 °C, this ratio decreased when the dwell time was increased from 2 to 4 h. This suggests that the rate of dissolution of Fe atoms exceeded the rate of incorporation of Mn atoms. This could lead to a delay in reaching peak hardness values during ageing at temperatures between 150 and 180 °C.
(4)
The peak hardness value obtained was 104 HV, following a solution treatment at 600 °C for 2 h and ageing at 160 °C for 12 h.

Author Contributions

J.A.-L. conceived and designed the investigation; A.C.-V. and A.G.-P. performed all laboratory work; F.A.-A. led the investigation, analysed the data, and wrote the paper. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. Outline of the experimental work carried out. OM: optical microscopy; DSC: differential scanning calorimetry; EDX: energy dispersive X-ray spectroscopy; SEM: scanning electron microscopy.
Figure 1. Outline of the experimental work carried out. OM: optical microscopy; DSC: differential scanning calorimetry; EDX: energy dispersive X-ray spectroscopy; SEM: scanning electron microscopy.
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Figure 2. Microstructure in the as-cast state. (a) Dendritic segregation is observed; (b) β-Al5FeSi particles at the grain boundaries. The etching reagent consisted of a solution of 100 mL distilled water with 4 g KMnO4 and 1 g NaOH.
Figure 2. Microstructure in the as-cast state. (a) Dendritic segregation is observed; (b) β-Al5FeSi particles at the grain boundaries. The etching reagent consisted of a solution of 100 mL distilled water with 4 g KMnO4 and 1 g NaOH.
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Figure 3. Microstructure in the as-cast state obtained under a scanning electron microscope (SEM) using electron channelling contrast imaging (ECCI). (a) It can be seen that the grain size can be estimated to be around 200–250 μm. (b) The β-Al5FeSi particles are in white and Mg2Si particles are in black.
Figure 3. Microstructure in the as-cast state obtained under a scanning electron microscope (SEM) using electron channelling contrast imaging (ECCI). (a) It can be seen that the grain size can be estimated to be around 200–250 μm. (b) The β-Al5FeSi particles are in white and Mg2Si particles are in black.
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Figure 4. Microstructure after solution treatments, employing quenching in water. (a) Treatment at 550 °C for 2 h. (b) Treatment at 550 °C for 4 h. (c) Treatment at 600 °C for 2 h. (d) Treatment at 600 °C for 4 h.
Figure 4. Microstructure after solution treatments, employing quenching in water. (a) Treatment at 550 °C for 2 h. (b) Treatment at 550 °C for 4 h. (c) Treatment at 600 °C for 2 h. (d) Treatment at 600 °C for 4 h.
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Figure 5. Microstructures obtained by scanning electron microscopy (SEM). (a) The as-cast state. The β-Al5FeSi particles and the Mg2Si phase can be observed, located at a grain boundary. (b) After a solubilization treatment at 600 °C with water cooling, which enabled the maximum solubilization of the Mg2Si phase and the transformation of the β-Al5FeSi particles into α-Al8(FeMn)2Si particles.
Figure 5. Microstructures obtained by scanning electron microscopy (SEM). (a) The as-cast state. The β-Al5FeSi particles and the Mg2Si phase can be observed, located at a grain boundary. (b) After a solubilization treatment at 600 °C with water cooling, which enabled the maximum solubilization of the Mg2Si phase and the transformation of the β-Al5FeSi particles into α-Al8(FeMn)2Si particles.
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Figure 6. Mean Fe/Si atomic ratio of AlFeSi particles after the different solution treatments (ST). The results are correlated with the atomic % of Mn in these particles. The “As Cast” state refers to the β-Al5FeSi particles, while the state after the solution treatment refers to the α-Al8(FeMn)2Si particles. The error bars show the distance between the mean value and the maximum and minimum values of the 30 particles analysed in each specimen.
Figure 6. Mean Fe/Si atomic ratio of AlFeSi particles after the different solution treatments (ST). The results are correlated with the atomic % of Mn in these particles. The “As Cast” state refers to the β-Al5FeSi particles, while the state after the solution treatment refers to the α-Al8(FeMn)2Si particles. The error bars show the distance between the mean value and the maximum and minimum values of the 30 particles analysed in each specimen.
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Figure 7. Mean (Fe + Mn)/Si atomic ratio of AlFeSi particles after the different solution treatments (ST). The atomic percentages of Si and Fe are also shown. The “As Cast” state refers to β-Al5FeSi particles, while the state after the solution treatment refers to the α-Al8(FeMn)2Si particles. The error bars show the distance between the mean value and the maximum and minimum values of the 30 particles analysed in each specimen.
Figure 7. Mean (Fe + Mn)/Si atomic ratio of AlFeSi particles after the different solution treatments (ST). The atomic percentages of Si and Fe are also shown. The “As Cast” state refers to β-Al5FeSi particles, while the state after the solution treatment refers to the α-Al8(FeMn)2Si particles. The error bars show the distance between the mean value and the maximum and minimum values of the 30 particles analysed in each specimen.
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Figure 8. Continuous heating DSC at 10 °C/min. The samples were previously aged naturally. The exothermic peaks (A and C) indicate precipitation of the β”-β’ and β phases, respectively. The endothermic peak (B) reflects the dissolution of the β”-β’ phases, precipitated in A.
Figure 8. Continuous heating DSC at 10 °C/min. The samples were previously aged naturally. The exothermic peaks (A and C) indicate precipitation of the β”-β’ and β phases, respectively. The endothermic peak (B) reflects the dissolution of the β”-β’ phases, precipitated in A.
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Figure 9. Hardness profiles after the ageing treatments. (a) Treatment at 550 °C for 2 h. (b) Treatment at 550 °C for 4 h. (b) Treatment at 600 °C for 2 h. (d) Treatment at 600 °C for 4 h.
Figure 9. Hardness profiles after the ageing treatments. (a) Treatment at 550 °C for 2 h. (b) Treatment at 550 °C for 4 h. (b) Treatment at 600 °C for 2 h. (d) Treatment at 600 °C for 4 h.
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Table 1. Chemical composition (% by weight).
Table 1. Chemical composition (% by weight).
%Si%Fe%Cu%Mg%Mn%Ti
0.420.220.0180.470.0310.019

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Alvarez-Antolin, F.; Asensio-Lozano, J.; Cofiño-Villar, A.; Gonzalez-Pociño, A. Analysis of Different Solution Treatments in the Transformation of β-AlFeSi Particles into α-(FeMn)Si and Their Influence on Different Ageing Treatments in Al–Mg–Si Alloys. Metals 2020, 10, 620. https://doi.org/10.3390/met10050620

AMA Style

Alvarez-Antolin F, Asensio-Lozano J, Cofiño-Villar A, Gonzalez-Pociño A. Analysis of Different Solution Treatments in the Transformation of β-AlFeSi Particles into α-(FeMn)Si and Their Influence on Different Ageing Treatments in Al–Mg–Si Alloys. Metals. 2020; 10(5):620. https://doi.org/10.3390/met10050620

Chicago/Turabian Style

Alvarez-Antolin, Florentino, Juan Asensio-Lozano, Alberto Cofiño-Villar, and Alejandro Gonzalez-Pociño. 2020. "Analysis of Different Solution Treatments in the Transformation of β-AlFeSi Particles into α-(FeMn)Si and Their Influence on Different Ageing Treatments in Al–Mg–Si Alloys" Metals 10, no. 5: 620. https://doi.org/10.3390/met10050620

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