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Article

Phase Diagram of Al-Ca-Mg-Si System and Its Application for the Design of Aluminum Alloys with High Magnesium Content

1
Department of Metal Forming, National University of Science and Technology MISiS, 4 Leninsky pr., 119049 Moscow, Russia
2
Institution of Russian Academy of Sciences A.A. Baikov Institute of Metallurgy and Material Science RAS, 49 Leninsky pr., 119991 Moscow, Russia
*
Author to whom correspondence should be addressed.
Metals 2017, 7(10), 429; https://doi.org/10.3390/met7100429
Submission received: 28 August 2017 / Revised: 29 September 2017 / Accepted: 9 October 2017 / Published: 13 October 2017

Abstract

:
The phase transformations in the Al-Ca-Mg-Si system have been studied using thermodynamic calculations and experimental methods. We show that at 10% Magnesium (Mg), depending on the concentrations of calcium (Ca) and silicon (Si), the following phases crystallize first (apart from the aluminum (Al) solid solution): Al4Ca, Mg2Si, and Al2CaSi2. We have found that the major part of the calculated concentration range is covered by the region of the primary crystallization of the Al2CaSi2 phase. Regardless of the Ca and Si content, the solidification of the aluminum-magnesium alloys ends with the following nonvariant eutectic reaction: L → (Al) + Al4Ca + Mg2Si + Al3Mg2. With respect to the temperature and composition of the liquid phase, this reaction is close to the eutectic reaction in the Al-Mg binary system. The addition of Ca and Si to the Al-10% Mg base alloy increases its hardness, reduces its density, and has no negative influence on its corrosion resistance. We have also established that the near-eutectic alloy containing about 3% Ca and 1% Si has the optimum structure.

1. Introduction

Aluminum-magnesium alloys are widely used in various products in the automotive industry, shipbuilding, rocket technology, and other important industries [1,2] due to a successful combination of their properties. In particular, their high plasticity and weldability are combined with low density and high corrosion resistance [3,4]. These alloys are non-heat treatable, but at high magnesium contents (about 10%, corresponding to the casting alloy 520), due to hardening of the aluminum solid solution (hereafter (Al)), the ultimate tensile stress (UTS) in the as-quenched state (T4) is up to 350 MPa–400 MPa [1,3].
It is advisable to alloy aluminum–magnesium alloys with silicon, which is included in a number of branded alloys (for example, 512) with a content of 1.5–2% [1,5,6,7]. Silicon (Si) maintains a low density (it forms, with magnesium (Mg), the Mg2Si phase, the density of which is only 1.88 g/cm3 [2]) and high corrosion resistance, while also increasing the hardness and casting properties of the alloy. A large number of works reported alloys based on the Al + Mg2Si eutectic, which have a structure typical of composites [8,9,10,11,12,13].
Another promising eutectic-forming element that can be considered a component for aluminum alloys is calcium. With respect to the content in the Earth’s core (3.6 wt %), calcium (Ca) occupies the third place among the metals, yielding only to aluminum and iron. Its density is 1.542 g/cm3, and as a result, its inclusion reduces the weight of aluminum alloys. In recent years, many publications have considered calcium as a component in magnesium-based alloys [14,15,16,17,18,19,20,21,22,23,24]. However, this element has not yet found a proper application in aluminum alloys [25,26,27].
The Al-Ca diagram is an eutectic type one [4,28,29,30]. However, unlike silicon, calcium does not form phases with magnesium (in the aluminum-rich region) [31]. The Al4Ca compound is in equilibrium with Al. However, in the Al-Ca-Si ternary system, there is the compound Al2CaSi2 [4,32,33], which does not allow the distribution of calcium and silicon between three possible phases (Al4Ca, Mg2Si and Al2CaSi2) in the quaternary Al-Ca-Mg-Si system. Thus, to assess the appropriateness of joint calcium and silicon alloying of the aluminum-magnesium alloys, analysis of the quaternary Al-Ca-Mg-Si system is required. In this system, calcium is the main eutectic-forming element, and it largely determines the castability of the alloys [30,34]. In addition, calcium can has a positive effect on corrosion resistance. Magnesium has a high solubility in aluminum, and enables considerable hardening at concentrations above 5% [2,3,4,35]. Silicon can enter into the composition of complex multicomponent eutectics with a fine structure, which can be favorable for mechanical properties. We expect that the new alloys will be useful for the production of shaped castings with low density and high corrosion resistance. The use of these composite alloys for the production of metallic glass is hardly possible due to the low glass-forming ability [36,37,38] determined by their chemical composition (in particular, a high content of magnesium and the absence of refractory transition metals).
As this quaternary system has not yet been studied in detail, the main aims of this study are as follows:
  • To study the phase diagram of the Al-Ca-Mg-Si system using thermodynamic calculations and experimental methods. It should be noted that the analysis of phase equilibria will be conducted with respect to conventional branded aluminum alloys technology of a liquid solidification, with a cooling rate range of 1–10 K/s.
  • To experimentally investigate the combined effect of Ca and Si additions on the structure, phase composition, and specific properties of Al-Mg alloys.
  • To identify and justify promising compositions for the development of new corrosion-resistant alloys with reduced density.

2. Materials and Methods

The objects of the experimental study were the Al4Ca12Mg, Al6Ca2.5Mg, Al10Ca10Mg2Si, Al4Ca10Mg2Si, Al3Ca10Mg1Si and Al10Mg alloys, the calculated phase compositions of which are considered below (Table 1).
The smelting was conducted in an electric resistance furnace (OOO LAC, Rajhrad, Czech Republic) in clay-graphite crucibles. All alloys were prepared using high purity Al (99.99%) with additions of pure alloying components of Ca 99.9%, Mg 99.9% and Si 99.9%. The melt was poured into a graphite mold at 730 °C–740 °C to produce flat castings with a size of 15 mm × 30 mm × 180 mm (the cooling rate during solidification was about 10 K/s). The chemical composition was controlled with an ARL 4460 optical emission spark spectrometer (Thermo Fisher Scientific, Waltham, MA, USA). The actual concentrations of Si, Cu, and Sn were very close to the nominal values.
The heat treatment of the castings was carried out in a SNOL muffle electric furnace (AB “UMEGA”, Utena, Lithuania) at 440 °C for 3 h followed by quenching in water (T4 temper). To evaluate the effect of the alloys composition on the distribution of Al3Mg2 precipitates, artificial aging at 200 °C was carried out for 3 h after quenching.
The structures of the as-cast and heat-treated samples were examined by means of optical (OM, Axiovert 200 MMAT, Carl Zeiss, Oberkochen, Germany) and scanning electron (SEM, TESCAN, VEGA 3, Tescan Orsay Holding, Brno, Czech Republic) microscopes, and by electron microprobe analysis (EMPA, OXFORD Aztec, Oxford Instruments, Oxfordshire, UK). The samples were cut from the castings, ground, and polished using conventional procedures. Mechanical polishing (Struers Labopol-5, Struers, Copenhagen, Denmark) was applied. The study of the fine structure, particularly for determining the precipitates of Al3Mg2 phase, was conducted under a transmission electron microscope JEM2100 (TEM, JEOL Ltd, Tokyo, Japan) at an accelerating voltage of 200 kV. The sample foil plates were cut from the ingots. The foil disks were thinned in a Struers device (Struers, Copenhagen, Denmark) for electrolytic preparation of specimens at a voltage of 15 V and a temperature of −40 °C in a chlorine-alcohol electrolyte solution (C2H5OH with 10% HClO4).
X-ray analysis was carried out on a Bede D1 System (Bruker, Karlsruhe, Germany) with Cu Kα radiation (λ = 0.15406 nm). The objects of the X-ray diffraction (XRD) study were fine powder specimens (up to 50 μm in diameter) cut from part of the ingots.
The Brinell hardness was determined in a INNOVATEST (series NEMESIS 9000, INNOVATEST, Maastricht, The Netherlands) hardness testing machine with a 2.5 mm diameter ball and a 612.9 N load for a 30 s dwell time.
The density was determined using the Archimedes method. The test sample was weighed on a HR-202i laboratory electronic scale in air (m1) and in water (m2). Then, the density was defined as:
ρ = m 1 ( ρ ω ρ a ) m 1 m 2 + ρ a
where ρω is the density of water, kg/m3; ρa is the density of air, kg/m3.
Tests for intergranular corrosion were carried out in a 3% solution of NaCl + 1% HCl solution at a temperature of 20 °C for 24 h.
Differential Scanning Calorimetry (DSC) with a heating and cooling rate of 10 K/min was performed using a high-temperature DSC Setaram Setsys Evolution (SETARAM Instrumentation, Caluire, France) on specimens with a mass of ~80 mg. The experiment was carried out in a dynamic Ar atmosphere with a flow rate of 50 mL/min. A temperature accuracy of ±0.5 °C was obtained.
We used the Thermo-Calc software (TTAL5 database [39]) to calculate the phase composition.

3. Results and Discussion

3.1. Analysis of Al-Ca-Mg-Si Phase Diagram

The TTAL5 database is designed to calculate the phase composition of multicomponent aluminum-based alloys, and contains the thermodynamic values of all the chemical elements of a given quaternary system and the expected phases: Al3Mg2, Al4Ca, Mg2Si, Al2CaSi2, (Si) [33,34]. The characteristics of these phases are given in Table 2.
Initially, on the basis of the calculation of phase equilibria, the general structure of this quaternary system in the Al-corner was proposed in the form of a polythermal diagram (projection of the solidification surfaces) [4,35]. According to Figure 1, three quaternary phase fields can be in the solid state: (Al) + Al3Mg2 + Al4Ca + Mg2Si, (Al) + Al4Ca + Mg2Si + Al2CaSi2, and (Al) + Mg2Si + Al2CaSi2 + (Si). Thus, the ternary compound cannot be in equilibrium with Al3Mg2. The fields correspond to the binary eutectic reactions (L → (Al) + β, where β is the second phase), the lines correspond to the ternary eutectics (L → (Al) + β1 + β2), and the points correspond to the invariant reactions. The temperatures of these invariant reactions, as well as the compositions of the liquid phase and (Al), are given in Table 3. In alloys with high magnesium content, there is a eutectic reaction L → (Al) + Al4Ca + Mg2Si + Al3Mg2, and another eutectic reaction is L → (Al) + Al4Ca + Mg2Si + (Si) in the alloys with high silicon content (points E1 and E2 in Figure 1, respectively).
In terms of temperature and phase composition, these five-phase reactions are close to the corresponding four-phase reactions in the Al-Mg-Si system (points e2 and e4 in Figure 1). The point P corresponds to the peritectic reaction L + Al2CaSi2 → (Al) + Al4Ca + Mg2Si. If we assume the existence of the quasi-ternary cross-section Al-Al2CaSi2-Mg2Si, then one more invariant reaction L → (Al) + Al4Ca + Mg2Si is possible in the quaternary system (point E3). Such situations are typical of some other quaternary systems, such as Al-Cu-Mg-Si and Al-Fe-Mg-Si [4,34].
Then, a qualitative analysis of phase transformations was performed using the calculated liquidus projections and vertical cross-sections. Finally, to obtain quantitative estimates, calculations of phase fractions and chemical compositions were performed at the temperatures of the phase transformations.
Since the primary crystals of the second phases are certainly undesirable, we calculated the liquidus surfaces. In the ternary Al-Ca-Mg system, with an increase in the magnesium content, the eutectic polytherm (corresponding to the reaction L → (Al) + Al4Ca) shifts toward the lower calcium concentrations (Figure 2a). On the basis of this polytherm, two ternary alloys—Al-4% Ca-12% Mg and Al-6% Ca-2.5% Mg, hereinafter Al12Mg4Ca and Al2.5Mg6Ca—were chosen for further consideration. According to their positions in the diagram (marked in Figure 2a), these alloys should have near-eutectic microstructures.
For the quaternary system, the liquidus projection was calculated at 10% Mg. It can be seen from Figure 2b that the major part of the calculated concentration range is covered by the region of the primary crystallization of the Al2CaSi2 phase. Even at high calcium contents, 1% Si is sufficient to make this ternary compound crystallize first (rather than Al4Ca). The areas of the primary crystallization of the Al4Ca and Mg2Si binary compounds are very narrow, and are located near the sides corresponding to the respective ternary systems (Al-Ca-Mg and Al-Mg-Si).
For the quantitative analysis of the phase composition, three quaternary alloys were chosen: Al-10% Ca-10% Mg-2% Si, Al-4% Ca-10% Mg-2% Si, and Al-3% Ca-10% Mg-1% Si (hereinafter Al10Mg10Ca2Si, Al10Mg4Ca2Si, and Al10Mg3Ca1Si, respectively). The positions of these alloys are shown in Figure 2b, from which it can be seen that the first two alloys fall into the region of primary crystallization of the Al2CaSi2 compound. In the Al10Mg3Ca1Si alloy, the primary crystals of the Ca- and Si-containing phase should not be formed, and the alloy should have a near eutectic microstructure. A general concept of the solidification character of quaternary alloys can be obtained from vertical sections, one of which is shown in Figure 3. The section calculated at 20% Mg and 1% Ca (Figure 3a) shows that the primary magnesium silicide crystals should form even at low silicon contents (less than 1%). The solidification of the alloys in this section containing up to ~3.5% Si should end with the invariant eutectic reaction L → (Al) + Al4Ca + Mg2Si + Al3Mg2, the parameters of which are presented in Table 3.
The most representative cross-section for the selected quaternary alloys is that for 10% Mg and 84% Al. It can be seen from Figure 3b that, in most alloys pertaining to this cross-section (where the total content of Ca and Si is constant and amounts to 6%), the solidification starts with the formation of the Al2CaSi2 compound. At 3% Ca and 3% Si, the liquidus temperature exceeds 650 °C, which is significantly higher compared with the boundary ternary alloys (Al-10% Mg-6% Si and Al-10% Mg-6% Ca). In the central region of the cross section, there is a horizontal line that corresponds to the invariant peritectic reaction L + Al2CaSi2 → (Al) + Al4Ca + Mg2Si (see Table 3). In alloys with an excess of silicon, this reaction ends with the disappearance of the liquid phase, i.e., such alloys complete the solidification in the four-phase region (Al) + Al4Ca + Mg2Si + Al2CaSi2. In alloys with a small amount of calcium, solidification ends with the monovariant eutectic reaction L → (Al) + Al2CaSi2 + Mg2Si. In this case, the solidus in this part of the polythermal section has a maximum (Figure 3b), which indicates an invariant nature of this eutectic reaction (for the alloy corresponding to the maximum point). This could confirm the assumption of the presence of a quasi-ternary Al-Al2CaSi2-Mg2Si cross-section in the Al-Ca-Mg-Si system (Figure 1).
In alloys with an excess of calcium, the ternary compound disappears as a result of an invariant peritectic reaction, and the solidification proceeds in accordance with the monovariant eutectic reaction L → (Al) + Al4Ca + Mg2Si, following which the alloy becomes three-phase. When the temperature is decreased, the Al3Mg2 compound is added to these phases as a result of the precipitation from (Al). It should also be noted that, even with the addition of negligible amounts of silicon to the Al-10% Mg-6% Ca boundary ternary alloy, magnesium silicide forms (Figure 3b) due to the very low solubility of Si in (Al). The vertical cross-section calculated at 3% Mg and 91% Al (Ca + Si = 6%) reveals a horizontal line (Figure 3c) corresponding to the invariant eutectic reaction L → (Al) + Al4Ca + Mg2Si + (Si) (see Table 3), which determines the end of solidification in low calcium alloys.
Calculation of the critical temperature of the selected alloys shows that they are very different from each other (Table 4). In particular, the liquidus temperatures differ by almost 150 °C, the Al10Mg10Ca2Si alloy has the highest value (729 °C), and the Al10Mg3Ca1Si alloy has the least (583 °C). According to the calculation, the quaternary alloys have the same phase composition in the solid state. In particular, as can be seen from Table 1, at 200 °C they contain four phases: (Al), Al4Ca, Mg2Si, and Al3Mg2. It should be noted that, even in the least alloyed Al10Mg3Ca1Si alloy, the total fraction of the second phases is ~35 vol %, which is typical for composites [40,41,42]. In the most alloyed Al10Mg10Ca2Si alloy, this fraction is more than half. At 440 °C (this value, as a rule, corresponds to the temperature of homogenization of Al-Mg alloys), the Al3Mg2 phase is absent, and the content of the Al4Ca and Mg2Si phases remains almost unchanged (as compared with 200 °C).
Since the actual solidification of most alloys is generally different from equilibrium, the evaluation of the phase composition of the casting or ingot in the as-cast state requires special techniques. One of the most commonly used techniques is the Scheil-Gulliver model, which is implemented in the Thermo-Calc program [33]. Figure 4 shows the nonequilibrium solidification curves (T-Q) calculated for the selected alloys using the given model. The Al-10% Mg alloy was considered as the reference one, and its T-Q curve is shown in Figure 4a. In the Al12Mg4Ca and Al2.5Mg6Ca ternary alloys, the eutectic reaction L → (Al) + Al4Ca starts almost immediately after the formation of the primary (Al) crystals (Figure 4b,c). The solidification of these alloys ends with the invariant reaction L → (Al) + Al4Ca + Al3Mg2. The difference between these alloys is that in the former alloy, more than 20% of the liquid phase solidifies by this reaction, and in the latter one, about 2%.
According to Figure 4d,e, in the Al10Mg10Ca2Si and Al10Mg4Ca2Si quaternary alloys, the first crystallizing compound was Al2CaSi2, which under equilibrium conditions should disappear as a result of the peritectic reaction. However, since the peritectic reactions, as a rule, do not complete during actual solidification of aluminum alloys [3], the presence of primary crystals of this ternary compound in the as-cast structure should be expected. It also follows from Figure 4d–f that the solidification of all alloys containing Ca and Si should be ended via the five-phase eutectic reaction, the parameters of which are given in Table 3.

3.2. Analysis of the Microstructure and Physical and Mechanical Properties

The main structural component of the as-cast Al4Ca12Mg and Al6Ca2.5Mg alloys is the (Al) + Al4Ca eutectic (Figure 5a,b), which corresponds to the position of the alloys on the liquidus projection of the Al-Ca-Mg system (Figure 2a). In the Al6Ca2.5Mg alloy, the eutectic is coarser than in the Al4Ca12Mg alloy (Figure 5c,d). In the Al4Ca12Mg alloy, the veins of the Al3Mg2 phase are also distinguished, which is also characteristic of binary alloys (type 520). The leading phase in the formation of a Ca-containing eutectic with a relatively fine structure is the Al4Ca compound, as seen from Figure 5a.
As we expected (see Figure 2b), the structure of the Al10Mg10Ca2Si and Al10Mg4Ca2Si hypereutectic alloys is characterized by the presence of primary crystals of Ca-containing compounds, which are clearly revealed in the optical microscope (Figure 6). These crystals are enriched with calcium and silicon (Figure 7). The results of a quantitative analysis of the composition of these crystals, which was carried for the largest particles, show that in the Al10Mg4Ca2Si alloy, they correspond sufficiently well to the compound Al2CaSi2 (Table 1). This experimental result agrees with the calculation according to which this particular ternary compound crystallizes first (Figure 4e). Some detectable amount of magnesium is probably associated with a high content of this element in the alloy and, as a consequence, with “backlighting”.
In the Al10Mg10Ca2Si alloy, the composition of the primary crystals (see Table 5) is close to the composition of Al4Ca aluminide (20 at %). The presence of silicon in this alloy (~4%) can be attributed to the fact that the solidification of this alloy begins with the formation of a ternary compound (containing silicon), which follows from the calculation (Figure 4d). The maximum quantity of the Al2CaSi2 phase primary crystals according to the calculation is only 3 wt %, which is several times smaller than the quantity of Al4Ca phase crystals that must form before the precipitation (Al). Presumably, the crystals of the ternary compound served as a substrate for the nucleation of binary aluminide crystals. Under equilibrium conditions, the ternary compound should disappear as a result of the peritectic reaction L + Al2CaSi2 → (Al) + Al4Ca + Mg2Si. However, this reaction being incomplete under actual solidification conditions, the conglomerates of two phases formed, and the composition of these conglomerates is shown in Table 5.
In the Al10Mg3Ca1Si alloy, whose structure is close to eutectic, no primary crystals of Ca- and Si-containing phases were detected (Figure 8a,b), which agrees with the results of the phase composition calculation (see Figure 2b and Figure 4e). The Al3Mg2 phase inclusions that are typical of the as-cast structure of the Al10Mg reference alloy (Figure 9a) are difficult to detect against the background of the eutectic alloy with a rather fine structure. During the 440 °C anneal, these inclusions dissolve, and as a result magnesium transfers to (Al). In the Al10Mg3Ca1Si alloy, the morphology of the Al4Ca eutectic phase particles varies slightly compared with the as-cast state. No evidence of fragmentation was revealed by TEM (Figure 8c). During the 200 °C heating, ~50 nm secondary Al3Mg2 precipitates form, and are distributed quite homogeneously (Figure 8d). In this alloy, there are no grain boundary chains of precipitates that are typical of the Al10Mg binary alloy after similar heat treatment (Figure 9b).
To experimentally determine the phase transformation temperatures, we conducted a DSC analysis of the experimental alloys (Figure 10). We found that the non-equilibrium solidus that corresponds to the reaction L → (Al) + Al4Ca + Mg2Si + Al3Mg2 is at about 450 °C. This temperature is very close to the calculated values (Table 4). The experimentally determined temperatures of the equilibrium solidus and liquidus are also fairly close to the calculated values. In particular, in the most alloyed Al10Mg10Ca2Si alloy, they are 730 °C and 500 °C, respectively. The presence of the Al4Ca compound in all Ca-containing alloys is confirmed by XRD data. This is illustrated, for example, by the X-ray diffraction patterns of the Al10Mg10Ca2Si and Al10Mg4Ca2Si hypereutectic alloys (Figure 11) in which this compound dominates (Table 1).
The determination of the density of the alloys shows that in all of the alloys with Ca and Si additives, it is less than that of the base binary alloy (Table 6). According to the corrosion resistance data, these additives do not have an adverse effect, as no weight loss or change in appearance was detected. The hardness of the as-quenched alloys (Table 6) is determined by the composition of the magnesium containing a supersaturated aluminum solid solution, and the fraction of eutectic phases (Table 1). The hardness of the Ca- and Si-containing alloys is much greater than that of the base alloy, due to the high percentage of the eutectic intermetallic phases. The presence of a significant amount of eutectic particles of Ca- and Si-containing phases suggests the possibility of increasing such characteristics that cannot be achieved in 520 type alloys. In particular, in the eutectic Al10Mg3Ca1Si alloy, the total amount of such phases is about 15 vol % (Table 1). In the Al10Mg10Ca2Si alloy where the percentage of the second phases is the highest and the density is the lowest (Table 6), the high brittle tendency should be expected due to a large number of primary crystals (Figure 6a).
The manufacturability of the experimental Al10Mg3Ca1Si alloy was evaluated in comparison with the base alloy Al10Mg. Grade alloys of the 5xx series have low casting properties due to a broad solidification range. The addition of silicon and calcium reduces this range and promises an increase in the casting properties. The high volume fraction of the brittle phases indicates low manufacturability for pressure treatment. Indeed, the deformability of the Al10Mg3Ca1Si alloy was not high. On the other hand, the Al2.5Mg6Ca alloy where the Al4Ca phase fraction is about 20 vol % showed sufficiently good manufacturability for hot and cold rolling. It can therefore be concluded that the eutectic inclusions of the Ca-containing phase are sufficient for achieving good processability.
Summarizing the results, we can assume that the A-Ca-Mg-Si system (in particular, the region near the Al10Mg3Ca1Si alloy) is quite suitable as a basis for the development of light corrosion resistant alloys with a «eutectic composite» type structure.

4. Conclusions

(1)
Using the calculation in the Thermo-Calc program, phase transformations in the Al-Ca-Mg-Si system in the region of aluminum-magnesium alloys have been studied. The structure of this quaternary system has been represented in the form of a polythermal projection (see Figure 1). The following phases can be in equilibrium with the aluminum solid solution: Al4Ca, Mg2Si, Al3Mg2, and Al2CaSi2.
(2)
In this quaternary system, three five-phase nonvariant reactions can occur: two eutectic, and one peritectic (see Table 3).
(3)
We show that the addition of calcium and silicon to the Al-10% Mg alloy can lead to the formation of primary crystals of the following phases: Al2CaSi2, Al4Ca, and Mg2Si. The formation of the ternary compound is most probable in this case.
(4)
In all the alloys considered, the solidification ends with the nonvariant eutectic reaction L → (Al) + Al4Ca + Mg2Si + Al3Mg20, the temperature and liquid phase composition of which are close to those of the reaction for the Al-Mg binary system.
(5)
It is established that the addition of Ca and Si in the Al-based alloy of 10% Mg increases hardness, reduces the density, and has no negative influence on the corrosion resistance.

Acknowledgments

The authors wish to acknowledge the financial support from the Ministry of Education and Science of the Russian Federation (Project No 11.7172.2017/8.9).

Author Contributions

Belov Nikolay Alexandrovich conceived and designed the experiments, conducted thermodynamic calculations, analyzed the results, wrote the paper (general edition); Naumova Evgenia Alexandrovna designed and performed the experiments, analyzed the results, wrote the part of the paper; Akopyan Torgom Karyoevich carried out of a part of thermodynamic calculations, performed the experiments, analyzed the results, wrote the part of the paper; Doroshenko Vitaliy Vladimirovich prepared samples and tools for experiments, performed the experiments, analyzed the results.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Polythermal projection of the Al-Ca-Mg-Si system in the aluminum corner.
Figure 1. Polythermal projection of the Al-Ca-Mg-Si system in the aluminum corner.
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Figure 2. The calculated liquidus projection of systems Al-Ca-Mg (a) and Al-Ca-Mg-Si (b) at 10 wt % Mg.
Figure 2. The calculated liquidus projection of systems Al-Ca-Mg (a) and Al-Ca-Mg-Si (b) at 10 wt % Mg.
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Figure 3. The calculated vertical cross sections of system Al-Ca-Mg-Si: (a) at 20% Mg and 1% Ca; (b) at 10% Mg and 84% Al (Ca + Si = 6%); (c) at 3% Mg and 91% Al (Ca + Si = 6%).
Figure 3. The calculated vertical cross sections of system Al-Ca-Mg-Si: (a) at 20% Mg and 1% Ca; (b) at 10% Mg and 84% Al (Ca + Si = 6%); (c) at 3% Mg and 91% Al (Ca + Si = 6%).
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Figure 4. The calculated Q-T curves (Sheil–Gulliver simulation) for the alloys: (a) Al10Mg; (b) Al12Mg4; (c) Al2.5Mg6Ca; (d) Al10Mg10Ca2Si; (e) Al10Mg4Ca2Si; (f) Al10Mg3Ca1Si.
Figure 4. The calculated Q-T curves (Sheil–Gulliver simulation) for the alloys: (a) Al10Mg; (b) Al12Mg4; (c) Al2.5Mg6Ca; (d) Al10Mg10Ca2Si; (e) Al10Mg4Ca2Si; (f) Al10Mg3Ca1Si.
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Figure 5. Microstructure of near-eutectic ternary alloys Al4Ca12Mg (a,c); and Al6Ca2.5Mg (b,d), scanning electron microscope (SEM) (Backscattered electrons (BSE)).
Figure 5. Microstructure of near-eutectic ternary alloys Al4Ca12Mg (a,c); and Al6Ca2.5Mg (b,d), scanning electron microscope (SEM) (Backscattered electrons (BSE)).
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Figure 6. Primary crystals of Ca-containing phases in hyper-eutectic quaternary alloys Al10Mg10Ca2Si (a) and Al10Mg4Ca2Si (b), optical microscope (OM).
Figure 6. Primary crystals of Ca-containing phases in hyper-eutectic quaternary alloys Al10Mg10Ca2Si (a) and Al10Mg4Ca2Si (b), optical microscope (OM).
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Figure 7. Electron microprobe analysis (EMPA) elemental mapping of Ca (a,b), Mg (c,d), and Si (e,f) in hyper-eutectic alloys Al10Mg10Ca2Si (a,c,e) and Al10Mg4Ca2Si (b,d,f).
Figure 7. Electron microprobe analysis (EMPA) elemental mapping of Ca (a,b), Mg (c,d), and Si (e,f) in hyper-eutectic alloys Al10Mg10Ca2Si (a,c,e) and Al10Mg4Ca2Si (b,d,f).
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Figure 8. Microstructure of alloy Al10Mg3Ca1Si. (a) OM, (b) SEM, (c,d) transmission electron microscope (TEM): (a) as-cast; (bd) solution treatment at 440 °C, 3 h; water quenching and aging at 200 °C, 3 h, (c) bright field, (d) dark field (Al3Mg2).
Figure 8. Microstructure of alloy Al10Mg3Ca1Si. (a) OM, (b) SEM, (c,d) transmission electron microscope (TEM): (a) as-cast; (bd) solution treatment at 440 °C, 3 h; water quenching and aging at 200 °C, 3 h, (c) bright field, (d) dark field (Al3Mg2).
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Figure 9. Microstructure of reference alloy Al10Mg: (a) as-cast, SEM (b) solution treatment at 440 °C, 3 h, water quenching and aging at 200 °C, 3 h, OM.
Figure 9. Microstructure of reference alloy Al10Mg: (a) as-cast, SEM (b) solution treatment at 440 °C, 3 h, water quenching and aging at 200 °C, 3 h, OM.
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Figure 10. DSC heating and cooling curves for the quaternary alloys: (a) Al10Mg10Ca2Si (b) Al10Mg4Ca2Si (c) Al10Mg3Ca1Si.
Figure 10. DSC heating and cooling curves for the quaternary alloys: (a) Al10Mg10Ca2Si (b) Al10Mg4Ca2Si (c) Al10Mg3Ca1Si.
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Figure 11. XRD patterns for the alloys Al10Mg10Ca2Si (a) and Al10Mg4Ca2Si (b).
Figure 11. XRD patterns for the alloys Al10Mg10Ca2Si (a) and Al10Mg4Ca2Si (b).
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Table 1. Calculated phase fractions for selected alloys of the Al-Ca-Mg-Si system.
Table 1. Calculated phase fractions for selected alloys of the Al-Ca-Mg-Si system.
AlloyT (°C)Phases
(Al)Al4CaMg2SiAl3Mg2
QM 1QV 2QM 1QV 2QM 1QV 2QM 1QV 2
Al10Mg10Ca2Si20043.4639.2036.9338.275.467.0714.1515.45
44057.7153.5036.8339.235.467.2700
Al10Mg4Ca2Si20067.9563.3614.7715.855.467.3211.9213.48
44079.9676.4814.5816.025.467.5000
Al10Mg3Ca1Si20069.6465.4811.0811.972.733.6916.5618.86
44086.3784.0110.9012.182.733.8100
1 QM—weight fraction, %. 2 QV—volume fraction, %.
Table 2. Characteristics of phases in the Al-rich alloys of Al-Ca-Mg-Si system [2,4,32,35].
Table 2. Characteristics of phases in the Al-rich alloys of Al-Ca-Mg-Si system [2,4,32,35].
FormulaCompositionCrystal LatticeDensity,
g/cm3
Hardness,
HV
wt %at %
Al4Ca27Ca20CaTetr. I4/mmm, 10 atoms/cell,
a = 4.36; Åc = 11.09 Å
2.35200–260
Mg2Si63.2Mg
36.8Si
66.7Mg
33.3Si
Cub. Fm3m, 12 atoms/cell
a = 6.35–6.40 Å
1.88450
Al3Mg237.3Mg40MgHex. Pm3m, 108 atoms/cell2.23200–340
Al2CaSi226.7Ca
37.3Si
20Ca
40Si
Hex. P3m1, 5 atoms/cell
A = 4.13; Åc = 7.15 Å
2.36 3?
(Si)100Si100SiCub. Fd3m a = 5.43 Å2.6870
3 Calculated.
Table 3. Calculated parameters of invariant reactions in the Al-Ca-Mg-Si system.
Table 3. Calculated parameters of invariant reactions in the Al-Ca-Mg-Si system.
ReactionPoint in Figure 1T, °CConcentration, wt %
PhaseAlCaMgSi
L → (Al) + Al4Ca + Mg2Si + Al3Mg2E1448L65.860.6733.380.08
(Al)84.090.0415.87<0.01
L → (Al) + Al2CaSi2 + Mg2Si + (Si)E2558L81.74<0.014.6713.59
(Al)98.00<0.010.641.35
L + Al2CaSi2 → (Al) + Al4Ca + Mg2SiP563L83.253.9312.000.83
(Al)95.340.334.290.64
L → (Al) + Al2CaSi2 + Mg2Si 4E3594L86.110.268.924.71
(Al)97.550.022.110.32
4 In quasi-ternary section.
Table 4. Calculated critical temperatures of selected alloys of the Al-Ca-Mg-Si system.
Table 4. Calculated critical temperatures of selected alloys of the Al-Ca-Mg-Si system.
AlloyTL, °CTS, °CΔT, °CTNS, °CΔTNS, °C
Al12Mg4Ca566463103448118
Al12.5Mg6Ca61058119448162
Al10Mg10Ca2Si729486243447282
Al10Mg4Ca2Si644521123447197
Al10Mg3Ca1Si58350578447136
Al10Mg60951396450159
Table 5. Chemical composition of primary crystals in alloys Al10Mg10Ca2Si and Al10Mg4Ca2Si.
Table 5. Chemical composition of primary crystals in alloys Al10Mg10Ca2Si and Al10Mg4Ca2Si.
AlloyConcentration, wt % (at %)Phase Identification
MgAlSiCa
10Mg4Ca2Si0.9 (1.1)35.8 (39.7)36.9 (39.4)26.4 (19.8)Al2CaSi2
10Mg10Ca2Si2.9 (3.5)64.5 (71.0)4.1 (4.3)28.6 (21.2)Al4Ca (+Al2CaSi2)
Table 6. Properties of experimental alloys 5.
Table 6. Properties of experimental alloys 5.
AlloyDensity, g/cm3Δm, %HB 6TL, °CTS, °CTNS, °C
Al12Mg4Ca2.530.075131---
Al2.5Mg6Ca2.480.02279---
Al10Mg10Ca2Si2.24-150785499450
Al10Mg4Ca2Si2.33-117647508451
Al10Mg3Ca1Si2.52<0.001119573500451
Al10Mg2.540.06297607511451
5 Δm—mass loss after corrosion test, TL—liquidus, TS—solidus, TNS—nonequilibrium solidus. 6 Hardness after quenching in water.

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Belov, N.A.; Naumova, E.A.; Akopyan, T.K.; Doroshenko, V.V. Phase Diagram of Al-Ca-Mg-Si System and Its Application for the Design of Aluminum Alloys with High Magnesium Content. Metals 2017, 7, 429. https://doi.org/10.3390/met7100429

AMA Style

Belov NA, Naumova EA, Akopyan TK, Doroshenko VV. Phase Diagram of Al-Ca-Mg-Si System and Its Application for the Design of Aluminum Alloys with High Magnesium Content. Metals. 2017; 7(10):429. https://doi.org/10.3390/met7100429

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Belov, Nikolay A., Evgenia A. Naumova, Torgom K. Akopyan, and Vitaliy V. Doroshenko. 2017. "Phase Diagram of Al-Ca-Mg-Si System and Its Application for the Design of Aluminum Alloys with High Magnesium Content" Metals 7, no. 10: 429. https://doi.org/10.3390/met7100429

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