3. Results
The study of the Fe-Si-Mn-Al system is one of the important tasks for obtaining an alloy with specified properties and characteristics, as well as for a correct understanding of the phase composition of the alloy at various ratios of iron, silicon, manganese and aluminum. In the Fe-Si-Mn-Al system under consideration, it is necessary to analyze 6 binary systems: Fe-Si, Fe-Mn, Fe-Al, Mn-Si, Al-Si, Al-Mn and 4 ternary systems: Fe-Si- Al, Si-Mn-Al, Fe-Mn-Si, Al-Mn-Si. All binary systems have been studied by numerous scientists [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27], and the phase diagrams are detailed.
In the system under consideration, one of the most common systems in the ferroalloy industry is the Fe-Si system. Melts of the Fe-Si system have been widely studied both experimentally and using various model representations. This allows them to be used as basic objects when testing new models and developing new methods for determining the thermodynamic properties of alloys.
More than 70 works of scientists around the world are devoted to the study of the state diagram of the Fe-Si system. In the alloys of the system, the existence of iron-based silicon solid solutions (γ-Fe and α-Fe), as well as intermetallic phases Fe
2Si(β), Fe
5Si
3 (η), FeSi (ε), FeSi
2 (NT) and FeSi
2 (VT), was discovered. which are presented in review papers [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27].
In the practical use of ferrosilicon, it was found that alloys containing at least 33.3% silicon are subject to dispersion. All alloys of this composition contain a ξ-phase - leboite, a phase of variable composition with a silicon content in the range of 52-58%, named «Leboit», at the suggestion of Kurnakov, in honor of the French scientist Lebo. This phase has two modifications: a high-temperature modification ξα and a low-temperature modification ξβ, which is similar in composition to the FeSi
2 compound, as follows from works [
31,
32].
It has been established that alloys containing the ξ-phase in the presence of aluminum, phosphorus and calcium additives are subject to disintegration [
33]. According to the authors, an important circumstance is that the alloys tend to fracture only in the simultaneous presence of aluminum and phosphorus, which is explained by the ability of aluminum and phosphorus, when dissolved in leboite, to form a quaternary solution of Fe-Si-P-Al. The solution, when exposed to air moisture, disintegrates with the release of hydrogen phosphide.
The decomposition of leboite is accompanied by a significant increase in its volume and is the cause of internal stresses that contribute to the disintegration of ferrosilicon. As the composition of the alloy moves away from the leboite phase (both in the direction of decreasing silicon content and in the direction of increasing it), the resistance of ferrosilicon increases, which is explained by a decrease in the amount of leboite in the alloy.
From the analysis of the phase diagram of the state of the Fe-Si system [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27], it follows that at a temperature of 298 K there are 5 intermetallic phases in the system: Fe
3Si, Fe
5Si
3, FeSi, FeSi
2, Fe
3Si. The initial data for the standard enthalpies of the Fe-Si system for thermodynamic diagram analysis are presented in
Table 2 (positions 1-5).
The phase diagram of the Fe-Al system is a component of ferrosilicoaluminum and ferroaluminum alloys. A large number of studies have been devoted to the Fe-Al phase diagram [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
34,
35]. The system includes five stable phases, namely: Fe
3Al, FeAl
2, FeAl, Fe
2Al
5, FeAl
3 and limited solid solutions on both the Fe and Al sides, each of which has its own homogeneity region (
Table 2 (positions 6-10).
A large number of works have been devoted to the Mn-Si phase diagram, as well as the above-mentioned phase diagrams; the most complete data are given in [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
36,
37,
38,
39].
There are seven intermetallic phases in the system: of these, Mn5Si3 and MnSi melt congruently at temperatures of 151,2 and 1542 K, respectively, ν(Mn9Si2), Mn3Si, Mn11Si19 are formed by peritectic reactions, R(Mn6Si) and Mn5Si - by peritectoid reactions. In addition, Mn3Si undergoes a polymorphic transformation at a temperature of 950 K.
The initial values of enthalpies of formation for manganese silicides, Mn
6Si, Mn
9Si
2, Mn
3Si, Mn
5Si
3, MnSi, Mn
2Si
3 and Mn
11Si
19 were taken from [
35] as the most reliable (
Table 2, positions 11-17).
The Al-Mn phase diagram is based on the results of the work of scientists given in [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
34,
40,
41,
42,
43,
44,
45]. The initial values of the standard enthalpies of formation of manganese aluminides - MnAl
6, MnAl
4, MnAl
3, Mn
4Al
11, MnAl were taken from [
34], as the most reliable ones were selected (
Table 2, positions 18-22).
A large number of studies have been devoted to the Al-Si phase diagram, a review of which was made in [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27,
45]. There are no intermetallic compounds in the Al-Si system, and a solid solution is formed throughout the composition. This system belongs to the simple eutectic type with low solubility of the components in each other in the solid state. Numerous results from various studies are in good agreement with each other. At a content of 12.3-12.7% there is a eutectic with a melting point of 850.2 K.
Information on the Fe-Mn phase diagram is given in [
14,
15,
16,
17,
18,
19,
20,
21,
22,
23,
24,
25,
26,
27] and reviewed in [
16]. It has been established that two peritectic invariant transformations occur in the alloys of the system. Calculation of the Fe-Mn phase diagram based on the thermodynamic properties of individual alloys of this system showed its good agreement with the diagram constructed from experimental data [
46,
47]. There are no chemical intermetallic compounds in the Fe-Mn system.
Ternary compounds in the Fe-Si-Mn-Al system have practically not been studied in relation to complex alloys. Scientific publications regarding this system are mainly devoted to aluminum coal with an aluminum content of more than 75-80%. As noted above, the Fe-Si-Mn-Al metal system consists of 4 ternary systems: Fe-Si-Al, Si-Mn-Al, Fe-Si-Mn, Fe-Mn-Al.
The latest reliable information about Fe-Si-Al is given in the author’s work [
48], where a fairly complete review of the compounds of this system was carried out based on data from works [
49,
50,
51]. The author of [
48] gives three types of triangulations of the Fe-Si-Al system with the presence of the FeAl
3Si
2 compound, which the author confirms by performing X-ray phase analysis. In fact, the author of [
48] confirmed the presence of the FeAl
3Si
2 compound in the TCAL database Fe
3Al
11Si
6, which in stoichiometry almost coincides with FeAl
3Si
2.
Thus, an analysis of the literature data shows that the Fe-Al-Si system contains stable ternary compounds, identified by microstructure and X-ray diffraction methods.
The value of ΔG°
298 for ternary compounds of the Fe-Al-Si system is not available in the literature, therefore, instead of the value of the standard Gibbs energy, the values of the standard enthalpy of formation of ternary compounds presented in
Table 3 [
48] were used in the calculation.
When carrying out triangulation of the Fe-Al-Si subsystem from double state diagrams of Fe-Si, Al-Si, Fe-Al and 7 ternary compounds Fe
xAl
ySi
z twenty-five areas were formed: 1) Si-Fe
3Si
7-F
2; 2) Fe
3Si
7-FeSi
2-F
2; 3) FeSi
2-FeSi-F
2; 4) FeSi-F
1-F
2; 5) FeSi-F
4-F
1; 6) F
1-F
4-F
2; 7) FeSi-F
3-F
4; 8) FeSi-FeAl-F
3; 9) FeSi-Fe
5Si
3-FeAl; 10) Fe
5Si
3-Fe
3Si-FeAl; 11) Fe
3Si-Fe
3Al-FeAl; 12) Fe
3Si-Fe-Fe
3Al; 13) FeAl-F
6-F
3; 14) F
3-F
4-F
6; 15) F
4-F
5-F
2; 16) F
5-F
6-F
2; 17) F
6-F
7-F
2; 18) F
4-F
6-F
5; 19) FeAl-FeAl
2-F
6; 20) FeAl
2-Fe
2Al
5-F
6; 21) Fe
2Al
5-FeAl
3-F
6; 22) FeAl
3-Al-F
6; 23) Al-F
7-F
6; 24) Al-Si-F
7; 25) Si-F
2-F
7 (
Figure 1).
Information about the conditions for the formation and stability of Si-Mn-Al ternary compounds is quite contradictory, and information about the structure obtained by various authors differs both in the number of phases and in the nature of phase equilibria between them [
35]. In total, the work considers nine ternary compounds Mn
4Al
3Si
2; Mn
3Al
3Si
2; Mn
3Al
3Si
4; Mn
3Al
8Si
9; Mn
4Al
9Si
3; Mn
3Al
9Si; Mn
3Al
12Si; Mn
2Al
9Si
2; Mn
3Al
15Si
2. Of these, in [
35] it is indicated that the Mn4Al3Si2 compound can undergo polymorphic transformations leading to cracking of the metal after crystallization, but they do not indicate the recrystallization temperature and the possible mechanism of formation of new compounds.
The value of ΔG°
298 for ternary compounds of the Si-Mn-Al system is not available in literature sources, therefore, the values of the enthalpies of formation were used for the calculation. The enthalpy of formation of ternary compounds of the Si-Mn-Al system was determined using the thermodynamic additivity method. The calculated values of the standard enthalpies of formation are given in
Table 4.
When triangulating the Si-Mn-Al subsystem from double state diagrams Al-Si, Al-Mn, Mn-Si and 9 ternary compounds Mn
xAl
xSi
x thirty-one areas were formed: 1) Mn-Mn
6Si-MnAl; 2) Mn
6Si-Mn
9Si
2-MnAl; 3) Mn
9Si
2-Mn
3Si-MnAl; 4) Mn
3Si-Mn
5Si
3-MnAl; 5) Mn
5Si
3-MnSi-MnAl; 6) MnSi-M
1-MnAl; 7) MnSi-M
3-M
1; 8) M
3-M
2-M
1; 9) MnSi-Mn
2Si
3-M
3; 10) Mn
2Si
3-Mn
11Si
19-M
3; 11) Mn
11Si
19-Si-M3; 12) Si-M
5-M
3; 13) Si-M
4-M
5; 14) Si-MnAl
4-M
7; 15) Si-M
8-M
7; 16) Si-M
9-M
8; 17) Si-Al-M
9; 18) M
8-M
9-M
7; 19) Al-M
9-M
7; 20) Al-M
7-MnAl
6; 21) MnAl
6-M
7-MnAl
4; 22) M
4-М
7-MnAl
4; 23) MnAl
4-M
4-M
5; 24) MnAl
4-M
5-M
6; 25) MnAl
4-M
6-MnAl
3; 26) MnAl
3-M
6-M
5; 27) MnAl
3-M
5-M
3; 28) MnAl
3-M
3-M
2; 29) MnAl
3-M
1-M
2; 30) MnAl
3-M
1-MnAl
11; 31) Mn
4Al
11-M
1-MnAl (
Figure 2).
There is no information about the presence of Fe-Mn-Si ternary compounds. When triangulating the Fe-Mn-Si subsystem, thirteen areas were formed from the double phase diagrams of Fe-Mn, Fe-Si and Mn-Si: 1) Fe-Mn-Mn
6Si; 2) Fe-Mn
6Si-Mn
9Si
2; 3) Fe-Mn
9Si
2-Fe
3Si; 4) Fe
3Si-Mn
9Si
2-Mn
3Si; 5) Fe
3Si-Mn
3Si-Mn
5Si
3; 6) Fe
3Si-Mn
5Si
3-MnSi; 7) Fe
3Si-MnSi-Fe
5Si
3; 8) Fe
5Si
3-MnSi-FeSi; 9) FeSi-MnSi-Mn
2Si
3; 10) FeSi-Mn
2Si
3-Mn
11Si
19; 11) FeSi- Mn
11Si
19-FeSi
2; 12) FeSi
2-Mn
11Si
19-Fe
3Si
7; 13) Fe
3Si
7-Mn
11Si
19-Si (
Figure 3).
There is also no information about the presence of ternary compounds in the Al-Mn-Fe system. When triangulating the Al-Mn-Fe subsystem, eleven areas were formed from the double phase diagrams of Al-Mn, Fe-Mn and Fe-Al: 1) Al-MnAl
6-FeAl
3; 2) MnAl
6-MnAl
4-FeAl
3; 3) MnAl
4-MnAl
3-FeAl
3; 4) MnAl
3-Fe
2Al
5-FeAl
3; 5) MnAl
3-FeAl
2-Fe
2Al
5; 6) MnAl
3-FeAl-FeAl
2; 7) MnAl
3-Fe
3Al-FeAl; 8) MnAl
3-Mn
4Al
11-Fe
3Al; 9) Mn
4Al
11-MnAl-Fe
3Al; 10) MnAl-Fe-Fe
3Al; 11) MnAl-Mn-Fe (
Figure 4).
Thus, the values of the enthalpy of formation in the Si-Mn-Al ternary system were calculated using the additive method. Binary systems (Fe-Si, Fe-Mn, Fe-Al, Mn-Si, Al-Si, Al-Mn) and ternary (Fe-Si-Al, Si-Mn-Al, Fe-Mn-Si and Al) systems are considered -Mn-Fe) systems.
Based on the tetrahedra of four particular three-component systems Fe-Si-Al, Si-Mn-Al, Fe-Mn-Si and Al-Mn-Fe, a diagram of the phase composition of the four-component system Fe-Si-Mn-Al was constructed (
Figure 5).
Table 5 presents a list of all elementary triangles of the studied systems.
As a result of calculations, elementary tetrahedra that make up this system were obtained. There are two methods for constructing a phase composition diagram. The first method is geometric, very complex for a given tetrahedron due to the large number of phases formed. As can be seen from
Table 5, it consists of 80 stable phase triangles. It is extremely difficult to draw all the connections correctly and not miss or not see the intersection of the boundaries of the triangles. Therefore, one of the methods of closing a triangle onto a tetrahedron was used.
This method consists of searching for triangles that have two identical phases “if two triangles from the nearest triple partial system have two identical phases, then they form a tetrahedron, etc.” According to
Table 5, we first consider the first two columns and find triangles that have two identical phases, and write them down. Next, we consider the phase compositions of the second and third columns. We also repeat finding two identical phases, etc. Following this method, fifty-six tetrahedra were obtained.
The breakdown of the general system was carried out for the most part taking into account congruent connections. The sum of the relative volumes of elementary tetrahedra is equal to unity (1.0).
Table 6 presents a list of elementary tetrahedra in the Fe-Si-Al-Mn system and their volumes relative to the volume of the original quaternary system, equal to 1 in arbitrary units.
The results of the calculations (
Table 6) confirm the reliability of the breakdown of the phase structure diagram of the Fe-Si-Mn-Al system.
Figure 6 shows the tetrahedron of the Fe-Si-Al-Mn quaternary system.
Based on the results of TDA and the constructed diagram of the real phase relationships in the Fe-Si-Mn-Al system, two regions of crystallization of leboite (Fe3Si7) were determined - the secondary and primary regions.
The secondary crystallization area of leboite belongs to the tetrahedron – Si-Fe
3Si
7-Mn
11Si
19-FeAl
3Si
2 (
Figure 6). Alloys having compositions in this area must be stable. Silicon atoms are primarily crystallized (t
mp = 1410°С). Crystallization of leboite (t
mp= 1205°С) occurs inside an already formed matrix of silicon crystals. Next, Mn
11Si
19 crystals begin to fall out (t
mp = 1155°С). Recrystallization of leboite according to the scheme Fe
3Si
7 → 3FeSi
2 + Si and an increase in volume by 17% occurs at 940°C. At this temperature, the FeAl
3Si
2 compound (t
mp ˂ 850°С) is in a liquid state. The presence of a framework of silicon crystals and still liquid FeAl
3Si
2 reduces the effect of internal stress and the increase in volume does not have a significant effect Therefore, with sufficiently rapid cooling, as is common in metallurgical practice, compositional alloys belonging to the Si-Fe
3Si
7-Mn
11Si
19-FeAl
3Si
2, area are not subject to destruction and further disintegration.
The primary crystallization region is characteristic of the region bounded by the FeSi
2-Fe
3Si
7-Mn
11Si
19- FeAl
3Si
2 tetrahedron (marked in blue), having a volume of 0.036933 ~ 3.7% (
Figure 6). Compositional alloys belonging to this area are unstable and tend to fracture. This range of compositions is characterized by primary crystallization of leboite (t
mp = 1205°С). Next, Mn
11Si
19 (t
mp = 1155°С) crystals begin to fall out. Meaning that, the frame of the alloy ingot is formed from Fe
3Si
7-Mn
11Si
19 crystals. Recrystallization of leboite at 940°C leads to an increase in internal stress due to an increase in volume, which leads to direct destruction of the ingot framework and the formation of numerous cracks. The formation of cracks in the ingot is the initial effect of destruction. Subsequently, atmospheric moisture interacts with excess phosphorus and calcium-containing phases with the release of gaseous products, which leads to complete disintegration of the alloy ingots.
Consequently, when planning and developing technology for smelting complex alloys based on Fe-Si-Mn-Al, it is necessary to regulate the initial compositions of the charge and the resulting alloy so as not to fall into the region of primary crystallization of leboite (Fe
3Si
7). The report [
27] indicates that the ternary compound Mn
4Al
3Si
2 (M1) has a tendency to polymorphic transformations during crystallization. However, this compound is not in the range of compositions of industrial alloys and was not considered by us.
Experiment
We verified the substantiation of the theoretical data obtained under experimental conditions using a large laboratory ore-thermal electric furnace with a transformer power of 200 kVA. The diameter of the graphite electrode is 150 mm. The electric furnace is two-electrode with a conductive hearth, and one electrode is coked in the hearth with the hearth mass. That is, the electric furnace has a structure similar to the Mige type electric furnace [
52,
53,
54]. The diameter of the furnace bath is 550 mm, the depth of the bath is 400-450 mm. The hearth of the furnace was made of carefully compacted and electrically conductive hearth mass. The transformer is powered by a voltage of 380 V. The electric furnace is equipped with four stages of secondary voltage regulation - from 18.4 to 49 V. The charge cone around the electrode was 0.3-0.45 m at an angle of 35-40°. The electric melting mode was chosen in such a way as to create the necessary temperature conditions in the shaft with deep seating of the electrodes, the current strength on the low side is from 2400 to 2800 A.
Manganese ore, high-ash coal and quartzite were used as raw materials for smelting the AMS alloy. Coke was not used due to the sufficient carbon content of coal.
The technical and chemical composition of the charge materials are presented in
Table 7 and
Table 8.
Smelting was carried out in a continuous manner, with periodic release of the alloy every 2 hours into cast iron molds. The process is a slag-free process. The charge was uniformly heated by the exhaust reaction gases, which created favorable conditions for the development of reduction processes. The reaction zone was characterized by high temperature, and the metal came out actively. Upon completion of the release of the melt, gases were rapidly released from the tap hole, which indicated the complete release of the metal from the reaction zone, after which fresh charge was loaded into the furnace to form a cone around the electrode [
55,
56,
57,
58,
59,
60].
The process of smelting a complex alloy: the release of the alloy and the formation of a cone from the charge around the electrode of the ore-thermal furnace are presented in
Figure 7.
Based on thermodynamic diagram analysis (TDA), we set the expected composition of the charge to obtain a complex AMS alloy with a content of 10-15% Fe; 40-50% Si; 30-40% Mn; 5-12% Al. The preliminary calculation was carried out by the iteration method, which is based on a numerical approximate method for solving technological problems using Microsoft Excel spreadsheets, and the charge was weighed: high-ash coal from the «Saryadyr» deposit - 20 kg; manganese ore from the «Bogach» deposit - 8 kg, quartzite - 2.53 kg. Quartzite was used in the charge mixture to adjust the chemical composition and neutralize residual carbon [
61,
62].
The resulting alloy of each release was weighed, after which samples were taken for chemical analysis. Chemical analysis of samples (
Table 9) was carried out in accordance with GOST-22772.4-77, GOST 22772.6-77, GOST 22772.7-96.
The maximum manganese content in this charge mixture is 40.96% in issue No. 9. The minimum manganese content is 30.2% in samples No. 13 and 14. The unweighted average manganese content in the alloy is 33.65%. Silicon in the alloy varies from 40.14 to 47.8%, the weighted average content is 45.01%. The weighted average content of aluminium in the alloy is 5.23%.
The practical application of the results of thermodynamic analysis to the smelting of the AMS complex alloy comes down to finding elementary tetrahedra within which their compositions are limited. To determine the manufacturability of the resulting alloys during the melting process, their chemical compositions were recalculated to the main elements of the Fe-Si-Mn-Al complex alloy, which are given in
Table 10.
The resulting prototypes of melts No. 4-7 and No. 10-18 of the AMS alloy after cooling and storage were stable and did not collapse. Experimental samples of the alloy melts No. 8 and No. 9 were destroyed and subsequently crumbled into fine powder.