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Article

Study of the Influence of the Thermal Capacity of the Lining of Acid Melting Furnaces on Their Efficiency

by
Viktor Alekseevich Kukartsev
1,
Vladislav Viktorovich Kukartsev
2,3,4,
Vadim Sergeevich Tynchenko
4,5,6,*,
Sergei Olegovich Kurashkin
4,6,7,
Roman Borisovich Sergienko
8,
Sergei Vasilievich Tynchenko
9,10,
Ilya Alexandrovich Panfilov
4,11,12,
Svetlana Vitalievna Eremeeva
7 and
Tatyana Aleksandrovna Panfilova
5
1
Department of Materials Science and Materials Processing Technology, Polytechnical Institute, Siberian Federal University, 660041 Krasnoyarsk, Russia
2
Department of Informatics, Institute of Space and Information Technologies, Siberian Federal University, 660041 Krasnoyarsk, Russia
3
Department of Information Economic Systems, Institute of Engineering and Economics, Reshetnev Siberian State University of Science and Technology, 660037 Krasnoyarsk, Russia
4
Digital Material Science: New Materials and Technologies, Bauman Moscow State Technical University, 105005 Moscow, Russia
5
Department of Technological Machines and Equipment of Oil and Gas Complex, School of Petroleum and Natural Gas Engineering, Siberian Federal University, 660041 Krasnoyarsk, Russia
6
Information-Control Systems Department, Institute of Computer Science and Telecommunications, Reshetnev Siberian State University of Science and Technology, 660037 Krasnoyarsk, Russia
7
Laboratory of Biofuel Compositions, Siberian Federal University, 660041 Krasnoyarsk, Russia
8
Machine Learning Department, Gini Gmbh, 80339 Munich, Germany
9
Department of Digital Control Technologies, Institute of Business Process Management, Siberian Federal University, 660041 Krasnoyarsk, Russia
10
Department of Computer Science and Computer Engineering, Institute of Computer Science and Telecommunications, Reshetnev Siberian State University of Science and Technology, 660037 Krasnoyarsk, Russia
11
Department of Systems Analysis and Operations Research, Reshetnev Siberian State University of Science and Technology, 660037 Krasnoyarsk, Russia
12
Department of Business Informatics and Business Process Modeling, Siberian Federal University, 660041 Krasnoyarsk, Russia
*
Author to whom correspondence should be addressed.
Metals 2023, 13(2), 337; https://doi.org/10.3390/met13020337
Submission received: 30 November 2022 / Revised: 2 February 2023 / Accepted: 3 February 2023 / Published: 8 February 2023

Abstract

:
First of all, the smelting equipment is the most important component of a foundry’s main production process and therefore requires constant reproduction. This is ensured by timely and high-quality maintenance and repair, the cost of which is 8–12% of the total costs. The technical and economic conditions of the enterprise itself depend on this, as the productivity of workers during production is directly related to the technical condition of the equipment and its downtime for repairs. An important factor in ensuring a melting furnace’s reproduction is a replacement of the worn lining, which leads to downtime of the smelting furnace and reduces the efficiency of its operation. The amount of torque required depends directly on the compound used. The quality of the manufacturing and sintering process of the lining, which provides the necessary durability, is affected by the heat capacity of the materials used when they are affected by the melting temperature of the alloys. In the present work, using the BRUKER D8 ADVANCE diffractometer, the Shimadzu XRF-1800 spectrometer and the STA 449 F1 Jupiter synchronous thermal analyzer, we probed the changes in the heat capacity of quartzite and PKMVI-3 under the action of temperatures of 200–1550 °C. This technology allows the manufacture of a lining that maintains high stability during operations at 1550–1600 °C melting modes.

1. Introduction

The manufacturing of castings is the most common process in forming part blanks due to its low cost and versatility of application. It makes it possible to obtain workpieces as close as possible to the profile of the future part and provide the necessary requirements for mechanical, physical, technical and special properties that are specified in the technical conditions [1]. This process can be applied to both individual and mass production. As of 2020, in Russia, various alloys and smelting equipment have been used for the production of castings, as shown in Figure 1.
Cast iron is the most common alloy, and induction furnaces are the most common furnace. Of the total number of induction crucible furnaces, about 18% are high-frequency induction furnaces designed for smelting alloy steel, and the rest are medium-frequency furnaces that can be used for smelting any alloy. The bulk of these are industrial-frequency induction crucible furnaces (ICFs), which have been in use since the middle of the last century [2,3,4].
First of all, the smelting equipment is the most important component of the foundry’s production base and requires constant reproduction. For this reason, a great deal of attention is being paid to improving the use of fixed assets, primarily related to the growth of return funds through improving the utilization of the equipment, improving the structure of fixed assets, modernization through improving the equipment and technology, and implementation of organizational and technical measures [5]. An important aspect of ensuring the functionality of a melting furnace is to replace the worn lining. Therefore, increasing the reliability of the smelter is one of the main tasks that ensures the necessary degree of reproduction of the main production facilities in order to comply with the following parameters of the aggregate: versatility in smelting alloys, performance, high lining durability, energy efficiency and maintenance costs [6]. Increased efficiency in the use of equipment is ensured by the adoption of new technologies that reduce downtime and reduce material inputs. The quality of the manufacturing process and the sintering of the lining affects its durability and, consequently, the efficiency of the melting furnace.
The main purpose of induction furnaces is the smelting of synthetic iron based on the use of scrap steel in the form of sheet trimmings, shavings and other metal waste with a small volume and weight. Figure 2 shows an image of an induction furnace at the moment of loading, with the main components labeled.
To make the furnace lining, the designers intended to use an acidic quartzite-based lining as the cheapest option, as its price is four–six times lower than the basic and neutral equivalents. The operation of these furnaces proved to be very robust, namely, 300–350 melts. The smelting of synthetic pig iron in these furnaces reduces its cost by 25–39% compared with the secondary smelting of iron [7,8,9]. This is particularly relevant in the current context, where all countries are facing the effects of the pandemic and the ensuing energy crisis [10].
The use of quartzite in the composition of refractory masses began in the second half of the 18th century for the manufacture of dyno products, which consisted of the linings of various heating and smelting furnaces [11,12,13,14]. Different types of quartzite differ in their mineral composition and content of elemental impurities (especially manganese, iron, aluminum, titanium, boron and phosphorus), the presence and concentration of which determine their industrial application and the possibility of further enrichment [15,16,17,18].
To obtain a lining with a high stability, it is necessary to use quartzite with a minimal number of impurities and a humidity of no more than 0.3%. However, manufacturers use wet enrichment to remove impurities. This includes washing operations, scrubbing, gravity, magnetic separation and flotation, resulting in a humidification of up to 2–3%. Therefore, the preparation of the lining of the induction furnace requires pre-drying with a further generation of the tridymite and cristobalite phases [19,20,21,22]. The tridymite produced during the drying of the quartzite and the subsequent sintering of the lining has been shown to maintain a constant volume at 840–1470 °C for a long time and thus provides the lining with a high resistance.
Based on the specificity conditions of service, the following basic requirements apply to the lining of the induction tiger furnaces, which are set out in the work [23].
When these requirements are met, three layers are formed in the lining after sintering, as shown in Figure 2.
Despite the fact that during the drying and sintering process the refractory materials undergo significant changes in their properties, after this process, the following three zones in the lining should be obtained: monolithic (sintered), semi-sintered and loose (Figure 3).
The boundaries of the transition from one zone to another are rather conventional, but in terms of their phase composition and thermophysical parameters, they all differ significantly from each other [24].
The phase composition of each zone is significantly influenced by the heat capacity of the formed elemental cells of the quartzite, which depend on the chemical and mineralogical composition of the initial material [25].
Traditional synthetic iron smelting technology requires a 30-degree liquid residue (bog) after discharge of 35% of the finished melting and melting temperatures not exceeding 1450 °C. The content limit of steel scrap is justified by its melting point since the melting point of carbon steel scrap is, depending on the chemical composition, 1400–1600 °C.

2. The Problem

At present, however, the situation in the market for cast iron castings has changed dramatically, as follows: cast iron scrap is virtually non-existent, and the cost of cast iron has increased dramatically, as has the cost of shipping it. This has led to the fact that synthetic cast iron can only be smelted in ICFs using increased amounts of steel scrap, carburizers and ferroalloys. However, to do this, it is necessary to raise the melting point above the allowable temperature for the furnace.
There is also a problem related to the persistence of the acid lining. The practice has shown that if the alloy is smelted at 1550 °C, the lining’s resistance decreases to 180 melts [26]. Replacing the acidic lining with a basic or neutral lining that can withstand this temperature causes it to cost 4–6 times more. The use of finished liner masses is advisable in medium-frequency furnaces where the inductor is fixed and the lining is not deformed. In ICFs, it is free and deformed during cyclic smelting modes and has been shown to be able to grow up to 50 mm by the end of the cycle, despite the periodicity of the tightening pins tightening the inductor’s turns. This type of deformation negatively affects the stability of the basic and neutral linings. In addition, the durability of the lining is affected by defects, which can be caused by a multitude of factors in its manufacture [27], sintering and slag mode [28]. This is influenced by the quality of the quartzite used and the manufacturing process of the lining mass.
As early as 1912, C. N. Fenner [29] established phase transformations in the quartzite when it was heated, in the form of a diagram scheme, according to which the tridymite phase is first and then the cristobalite phase. This was reflected in other studies [30,31]. Later, many studies disproved this pattern, which was explained by the emergence of the method of X-ray and the development of physico-chemical methods in the final 60–70 years of the last century. For this reason, since 1961, in studies of the phase transformations of quartzite when heated, tridymite has not been detected [32,33,34,35]. Spiker proposed a variant of the modified SiO2 diagram when heated to 1550 °C [36]. In addition, some studies have highlighted the regularity of the appearance of cristobalite first and then tridymite [37,38,39,40,41,42]. It was then established that the transformation to cristobalite begins at a prolonged temperature of 1000 °C, and at 1250–1450 °C, the process is intensified [43]. This process is also influenced by impurities in the source material [44]. Other studies have established the obligatory presence of a mineralizer to obtain the tridymite phase [45,46].
However, it must be considered that phase transformations occur with the release of heat and are accompanied by the emergence of a sparser aggregate state; that is, an increase in the volume and a reduction in the density due to the expansion of the crystal lattice [47]. In addition, phase transformations can be accompanied by both reductions in volume and heat release. The thermal stability of the melting furnace is estimated by the number of melts, and each melting (in the case of a 2.5 t furnace) is the heating of the lining after sintering to 1550 °C, then the melting mode occurs at 1550–1600 °C, and the temperature drops to 1450–1470 °C to drain the first portion of the alloy. After this, the second batch of metal is drained; during this time, the temperature of the lining layer is released when draining the first batch of metal reaches 1025 °C. After all the metal has been drained, the fresh metal filling is loaded, and the temperature of the lining is 800–900 °C. Everything is repeated until the lining has been completely worn. Under these conditions, changes in the structure of the quartzite are significantly influenced by the heat capacity of the initial material used, which is directly dependent on the resulting phase state.
The quantitative content of the different phases in the quartzite, when exposed to the repeated heating and cooling temperatures necessary for melting, affects the heat capacity of the lining itself and its durability.
Therefore, the study of changes in the heat capacity of the quartzite, which affects the stability of the applied lining when the melting temperatures are above 1450 °C, is an urgent task.

3. Materials and Methods

The study was carried out for quartzite (PKMVI-3V brand), with a humidity of 3.5%, supplied by JSC “DINUR”. According to the supplier, the finished product mainly contains quartz but also includes impurities of chalcedony, carbonates, opals and clay minerals, with a low concentration of iron oxides and high dispersion. The company, according to TU 1511-022-00190495-2003, guarantees the chemical composition presented in Table 1 (the contents of the remaining impurities are not given). In addition, the following grain composition is guaranteed, in mass proportions: remaining on grid No. 2, 6–15 inclusive; remaining on grid No. 3.2, not more than 5; passing through grid No. 0.5, 50–59 inclusive; passing through grid No. 0.1, 31–41.
The Shimadzu XRF-1800 X-ray fluorescence spectrometer (Shimadzu, Japan) was used to determine the chemical composition. The device was equipped with collimators and a built-in digital camera. The rotation speed of the sample was 60 rev/min.
Phase composition studies were carried out using the BRUKER D8 ADVANCE diffractometer (Bruker, Germany). The copper anode X-ray tube was used, and the diffraction spectrum was recorded by the VÅNTEC-1 high-speed positional detector.
The STA 449 F1 Jupiter (NETZSCH, Germany) was used for thermal analysis of the quartzite.
Earlier studies of changes in the structure of the quartzite at different temperatures used to remove the moisture in the original material showed their influence on the formation of phases under the influence of the temperatures necessary for sintering the lining [48]. For this reason, the following research methodology was adopted:
  • We determined the chemical composition of the quartzite, taking the presence of concomitant impurities into account;
  • The raw quartzite portion was heated to a temperature of 800 °C, given an exposure of 1 h and cooled to room temperature, then subjected to subsequent heating with exposure at each test point to remove the card and determine the parameters of the crystal lattice at uniform temperatures suitable for sintering and operating melting;
  • The next batch of raw quartzite was heated to a temperature of 200 °C, given an exposure of 1 h and cooled to room temperature. We then performed the same heating mode as in Step 2;
  • We investigated the change in the heat capacity of the quartzite using different moisture removal technologies (as in Steps 2 and 3), followed by heating corresponding to the sintering temperatures of the lining and several melting cycles.
The temperatures selected for this study were based on the following:
  • Between 200 and 800 °C, the approximate temperature for removing free moisture;
  • 600 °C, intensive phase conversion with heat release, applied during operation [49];
  • 1550–1600 °C, melting mode, for carburizing, alloying and modifying operations;
  • 1450–1470 °C, first alloy discharge;
  • 1025 °C, temperature of the released lining layer after the first discharge (at this time the second portion of the alloy is drained);
  • 800–900 °C, the temperature of the lining after discharging all the metal, when fresh metal filling is loaded.

4. Results and Discussion

Since the process of phase formation under temperature is affected by the number of impurities in the quartzite itself, the chemical composition of the quartzite was first analyzed using the Shimadzu XRF-1800X-ray fluorescent wave dispersion spectrometer. As a result of this analysis, it was found that the quantity of SiO2 was 96.54% instead of 97.5%, the quantity of Al2O3 was 0.982% instead of 1.1%, the CaO content was 0.189% instead of 0.089%, and Fe2O3 amounted to 0.93%, which is significantly more than declared, and the number of uncharged impurities was 0.638%. The results of the analysis are shown in Table 1.
The study of changes in the structure of the quartzite was carried out with the BRUKER D8 ADVANCE diffractometer, equipped with a Bragg–Brentano focus and an HTK 16 high-temperature chamber. The imaging took place at the angles of 2Θ = 10–90° in increments of 0.007; the duration of the imaging was 1 h.
Figure 4 shows the structure of a quartzite lattice at 1550 °C, pre-treated to remove moisture at 800 °C.
The diffractogram of quartzite pre-treated at 200 °C and subsequently heated to 1550 °C is shown in Figure 5.
To decipher the results of the study of the changes in the structure of the quartzite, the available databank was used in the form of cards of elementary cells with their characteristics (Table 2).
The parameters of the changes in the structure of the quartzite that occurred during the rise of the set temperatures were determined as follows. All the diffractograms taken counted the total number of crystalline phases, the content of which was not less than 5% and 100% were selected. The fraction of each crystalline phase was then determined, and its mean values were calculated, where davg is the average intergloss distance, Davg is the average density, Vavg is the average volume and Mavg is the average molecular mass of the lattice.
The results of the average characteristics of the parameters of the quartzite (including the phase composition) exposed to different temperatures for the removal of moisture and at the temperatures specified in the study are presented in Table 3.
In the numerator, values are given for quartzite treated at 200 °C; the denominator gives the values for quartzite treated at 800 °C. davg is the average interval–skeleton distance, Davg is the average density, Vavg is the average volume and Mavg is the average molecular mass of the grid.
The study of changes in the thermal capacity of quartzite was carried out on the NETZSCH STA 449C Jupiter instrument during thermal analysis. The heating rate was 10 K/min, and the collection speed of the points was 100 p/min. Two corundum crucibles were used for the measurements, one of which contained an experimental specimen and the other was used as a reference. High measurement accuracy ensured the maximum uniform distribution of the examined material in the crucible [50].
The aim was to study changes in the heat capacity of the quartzite at the temperatures experienced by the lining during the melting cycles immediately after the sintering process (three melting cycles were investigated). As a result, the thermograms were obtained (Figure 6 and Figure 7).
The heat capacity values are summarized in Table 4.
Using the values shown in Table 4, the heat capacity of the quartzite was plotted as shown in Figure 8.
The values of the heat capacity in each melting cycle were selected, and graphs of their changes were constructed. These are presented as fragments of thermograms in Figure 9, Figure 10, Figure 11, Figure 12, Figure 13 and Figure 14 for each type of quartzite.
On the presented fragments of the first smelting cycle shown in Figure 9 and Figure 10, it is evident that the heat capacity of the quartzite with pre-treatment of 200 °C is 2 times lower.
On the presented fragments of the second melting cycle, shown in Figure 11 and Figure 12, it is evident that the heat capacity of the quartzite with a preliminary temperature treatment of 200 °C is 2.3 times lower.
On the presented fragments of the third melting cycle, shown in Figure 13 and Figure 14, it is evident that the heat capacity of the quartzite with a preliminary temperature treatment of 200 °C is lower by 1.5 times.
All the thermograms have different colors for the cooling and heating periods during imaging.
In addition, based on the thermograms shown in Figure 6 and Figure 7, Table 5 of the enthalpy values for the studied quartzites has been compiled.
Based on these data, a graph of the changes in the enthalpy of quartzites is shown in Figure 15.
Studies have found that, despite the presence of 0.638% impurities in the quartzite, its preliminary calcination at a temperature of 800 °C and further cooling allowed the process of further sintering of the chalcedony lining based on it. At 1550 °C, we simultaneously obtained the following three phases: hexagonal quartzite + tridymite + cristobalite. Its structure consisted of elementary cells corresponding to 82% of the tridymite phase, 9% of cristobalite and 9% of hexagonal quartzite, and it had an average volume of Vav of 1606.96 Å3 (Table 3).
The resulting enthalpy graph showed that at this point, the heat absorption process of the sintered layer exceeded the heat absorbed into the next lining layer by 72%. During subsequent melting cycles, the fraction of tridymite increased and thus the average volume also increased, and the heat transfer process began to exceed its absorption by 1.5- to 4-fold (Figure 15). The heat capacity graph shows that after sintering, the heat capacity of the liner (ΔCp) was 0.037 J/K, and in subsequent melting cycles, it was characterized by λ-shaped jumps of between 0.05 and 0.045 J/K (Figure 8).
After completion of the sintering mode of the lining at 1550 °C, the structure of the quartzite pre-processed at 200 °C consisted of elementary cells. The corresponding phases were 26% cristobalite and 74% hexagonal quartzite and had an average volume of 143.65 Å3 (Table 3). The resulting enthalpy graph shows that at this point, the heat absorption process of the sintered layer exceeded the heat absorbed into the next lining layer by 62%. In subsequent melting cycles, the fraction of cristobalite increased, and thus, the average volume also increased, and the absorption process is 59% (second cycle) and 57% (third cycle). The heat capacity graph shows that after sintering, the heat capacity of the liner (ΔCp) was 0.018 J/K; in subsequent melting cycles, the liner was characterized by λ-shaped jumps of between 0.04 and 0.02 J/K (Figure 8).
The results of the changes in the heat capacity of the quartzite with different temperature treatments are shown in Figure 9, Figure 10, Figure 11, Figure 12, Figure 13 and Figure 14. Of these, it can be seen that the quartzite with a temperature treatment of 200 °C, after each cycle, the heat capacity is significantly lower than when processing 800 °C.
Thus, changes in the heat capacity and heat transfer and absorption were influenced by phase changes in the quartzite under the influence of temperature. Quartzite is known to be stable at 870–1470 °C, has a density of 2.3 g/cm3 and a hardness of 6.5 units on the Mohs scale. Cubic cristobalite is stable at a temperature of 1470–1715 °C, has a hardness of 7.25 units and has a density of 2.27 g/cm2 [51]. The greater hardness of the lining makes it more resistant to intense melting movement at elevated melting temperatures.
Based on this technology, in the foundry of a machine-building enterprise equipped with industrial frequency induction smelters of 1 and 2.5 tons, the process of smelting synthetic iron on one steel scrap was developed, including the manufacture of the lining itself with reference to existing equipment. Work during the month showed a positive result—the resistance of the lining on all p-hours was 320–340 melts. Based on this, the technology was adopted as the main one, and the results during the year showed that the resistance of the lining on the smelting furnaces, stable, amounted to 320–360 melts. An analysis of the use of raw materials was carried out and compared with the previous technology. For metal filling containing 30% of steel scrap, the following materials were purchased: 15% (150 kg) of cast iron at 40 rubles/kg at 6000 rubles; 1% (10 kg) of ferro-manganese and ferrosilization at 50 rubles/kg at 500 rubles; 30% (300 kg) steel scrap at a price of 10 rubles/kg in the amount of 3000 rubles and 0.6% (0.6 kg) carburizer at a price of 3 rubles/kg in the amount of 1.8 rubles.
The rest of the metal residue consisted of the return of production and the liquid residue in the kiln, the notional cost of 1 ton, which is 50% for the liquid residue and for the return of 80% SCH20 (Grey Cast Iron, GG-20 in Germany)—70 rubles/kg (330 · 35 = 11,500 rubles and 200 · 56 = 11,200 rubles).
The total cost amounted to 32,201.8 rubles/t liquid. For the smelting of 1 ton of liquid, when used in the meteor mill 88% of steel scrap, the costs amounted to the following: 1.5% ferrosile in the amount of 750 rubles; 100 kg liquid residue at the price of 5000 rubles; 88% of scrap steel in the amount of 8800 rubles and 2% carburizer in the amount of 6 rubles. The total cost of buying fresh materials amounted to 14,556 rubles. The calculation uses the market value of the materials as of 2018–2019.

5. Conclusions

According to these results, the sintered lining layer consisting of cristobalite and hexagonal quartzite, compared with a similar layer consisting mainly of tridymite, had a smaller average volume, its heat capacity at 1550 °C during the second and third melting cycles was 1.2–2 times lower, and the heat absorption process exceeded the heat transfer from the sintered to the semi-finished layer by 50%. In a sintered layer consisting of tridymite and quartzite, the process of heat transfer exceeded its absorption by 1.5–4 times, resulting in a more intensive change in the structure of the layers by accelerating the conversion of the half-melted material into filaments. This reduced the thickness of the lining, speeding up wear and thus reducing its durability.
Thus, research has shown that the acid lining, which has a lower heat capacity, has a higher hardness and, therefore, increased resistance to the intense movement of the melt, which will allow it to maintain its high resistance at melting temperatures up to 1470–1570 °C. This ensures the possibility of use in metal filling 90% or more, one steel scrap, reduces material and energy costs and increases productivity by reducing the downtime associated with the furnace. Based on the results of the research, the technology for manufacturing such a lining has been developed and proposed, including the main operations described below.
For the operation of removing moisture from the original raw material, it is necessary to make it use a temperature of 200 °C with subsequent cooling. The sintering process must be finished at a temperature of 1550–1570 °C with an exposure of 2 h. The first 3–5 melts are carried out with 1/3 of the capacity of the crucible and only then go to the necessary melting mode.
In this way, the efficiency of using a sheet consisting of quartzite and cristobalite, which has a low heat capacity, allows the use of metal filling with 88% of steel scrap and provides a 45.2% reduction in the cost of raw materials.

Author Contributions

Conceptualization, V.A.K., V.V.K., V.S.T. and S.O.K.; methodology, V.A.K., V.V.K., V.S.T. and S.O.K.; validation, S.V.T., I.A.P., R.B.S., S.V.E. and T.A.P.; formal analysis, V.A.K., S.V.T., I.A.P., S.V.E. and T.A.P.; investigation, V.S.T., S.O.K., R.B.S., S.V.T. and S.V.E.; resources, V.A.K., V.V.K., V.S.T. and I.A.P.; data curation, V.A.K., V.V.K., V.S.T., S.O.K. and S.V.T.; writing—original draft preparation, V.A.K., V.V.K., V.S.T., S.O.K., R.B.S., S.V.T., I.A.P., S.V.E. and T.A.P.; writing—review and editing, V.A.K., V.V.K., V.S.T., S.O.K., R.B.S., S.V.T., I.A.P., S.V.E. and T.A.P.; visualization, V.A.K., V.V.K., R.B.S., S.V.T. and I.A.P.; supervision, V.S.T., S.O.K., S.V.E. and T.A.P.; project administration, V.A.K., V.S.T. and S.O.K.; All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Distribution of foundries.
Figure 1. Distribution of foundries.
Metals 13 00337 g001
Figure 2. Induction melting furnace: 1—drain sock; 2—furnace cover; 3—gas atmosphere; 4—scrap metal; 5—inductor; 6—case.
Figure 2. Induction melting furnace: 1—drain sock; 2—furnace cover; 3—gas atmosphere; 4—scrap metal; 5—inductor; 6—case.
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Figure 3. Scheme of the furnace indicating the zones of the lining: 1—the bulk layer; 2—the semi-welded layer; 3—the sintered layer; 4—the furnace inductor; 5—the metal load; 6—the polished layer; 7—the furnace body.
Figure 3. Scheme of the furnace indicating the zones of the lining: 1—the bulk layer; 2—the semi-welded layer; 3—the sintered layer; 4—the furnace inductor; 5—the metal load; 6—the polished layer; 7—the furnace body.
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Figure 4. The structure of the quartzite consists of elementary cells of cristobalite, marked with purple color (card 01-085-0621); tridymite, marked with yellow (card 00-018-1170) and cells of quartzite, marked in red (card 01-071-0911).
Figure 4. The structure of the quartzite consists of elementary cells of cristobalite, marked with purple color (card 01-085-0621); tridymite, marked with yellow (card 00-018-1170) and cells of quartzite, marked in red (card 01-071-0911).
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Figure 5. The structure of quartzite consists of elementary cells of cristobalite (colored purple, cards 00-011-0695) and quartzite (colored red, cards 01-071-0911).
Figure 5. The structure of quartzite consists of elementary cells of cristobalite (colored purple, cards 00-011-0695) and quartzite (colored red, cards 01-071-0911).
Metals 13 00337 g005
Figure 6. Thermogram of quartzite, calcified at 800 °C (Av, average heat capacity).
Figure 6. Thermogram of quartzite, calcified at 800 °C (Av, average heat capacity).
Metals 13 00337 g006
Figure 7. Thermogram of a quartzite, calcified at 200 °C and sintered with an induction furnace’s lining.
Figure 7. Thermogram of a quartzite, calcified at 200 °C and sintered with an induction furnace’s lining.
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Figure 8. Thermal temperature dependence graph: a, quartzite treated at 200 °C; b, quartzite treated at 800 °C.
Figure 8. Thermal temperature dependence graph: a, quartzite treated at 200 °C; b, quartzite treated at 800 °C.
Metals 13 00337 g008
Figure 9. Fragment of the thermogram of quartzite, calcified at 200 °C (Cycle 1), where: Metals 13 00337 i001—cooling up to 1470 °C, Metals 13 00337 i002—heating up to 1025 °C, Metals 13 00337 i003—cooling up to 870 °C, Metals 13 00337 i004—cooling up to 1550 °C, Metals 13 00337 i005—drainage at 1470 °C, Metals 13 00337 i006—heating up to 1470 °C, Metals 13 00337 i007—heating up to 1550 °C, Metals 13 00337 i008—drainage at 1550 °C.
Figure 9. Fragment of the thermogram of quartzite, calcified at 200 °C (Cycle 1), where: Metals 13 00337 i001—cooling up to 1470 °C, Metals 13 00337 i002—heating up to 1025 °C, Metals 13 00337 i003—cooling up to 870 °C, Metals 13 00337 i004—cooling up to 1550 °C, Metals 13 00337 i005—drainage at 1470 °C, Metals 13 00337 i006—heating up to 1470 °C, Metals 13 00337 i007—heating up to 1550 °C, Metals 13 00337 i008—drainage at 1550 °C.
Metals 13 00337 g009
Figure 10. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 1), where: Metals 13 00337 i009—cooling up to 1470 °C, Metals 13 00337 i010—heating up to 1025 °C, Metals 13 00337 i011—cooling up to 870 °C, Metals 13 00337 i012—cooling up to 1550 °C, Metals 13 00337 i013—drainage at 1470 °C, Metals 13 00337 i014—heating up to 1470 °C, Metals 13 00337 i015—heating up to 1550 °C, Metals 13 00337 i016—drainage at 1550 °C.
Figure 10. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 1), where: Metals 13 00337 i009—cooling up to 1470 °C, Metals 13 00337 i010—heating up to 1025 °C, Metals 13 00337 i011—cooling up to 870 °C, Metals 13 00337 i012—cooling up to 1550 °C, Metals 13 00337 i013—drainage at 1470 °C, Metals 13 00337 i014—heating up to 1470 °C, Metals 13 00337 i015—heating up to 1550 °C, Metals 13 00337 i016—drainage at 1550 °C.
Metals 13 00337 g010
Figure 11. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 2), where: Metals 13 00337 i017—cooling up to 1550 °C, Metals 13 00337 i018—drainage at 1470 °C, Metals 13 00337 i019—cooling up to 1470 °C, Metals 13 00337 i020—cooling up to 870 °C, Metals 13 00337 i021—heating up to 1025 °C, Metals 13 00337 i022—heating up to 1550 °C, Metals 13 00337 i023—heating up to 1470 °C.
Figure 11. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 2), where: Metals 13 00337 i017—cooling up to 1550 °C, Metals 13 00337 i018—drainage at 1470 °C, Metals 13 00337 i019—cooling up to 1470 °C, Metals 13 00337 i020—cooling up to 870 °C, Metals 13 00337 i021—heating up to 1025 °C, Metals 13 00337 i022—heating up to 1550 °C, Metals 13 00337 i023—heating up to 1470 °C.
Metals 13 00337 g011
Figure 12. Fragment of the thermogram of quartzite, calcified at a temperature of 800 °C (Cycle 2), where: Metals 13 00337 i024—cooling up to 1550 °C, Metals 13 00337 i025—drainage at 1470 °C, Metals 13 00337 i026—cooling up to 1470 °C, Metals 13 00337 i027—cooling up to 870 °C, Metals 13 00337 i028—heating up to 1025 °C, Metals 13 00337 i029—heating up to 1550 °C, Metals 13 00337 i030—heating up to 1470 °C.
Figure 12. Fragment of the thermogram of quartzite, calcified at a temperature of 800 °C (Cycle 2), where: Metals 13 00337 i024—cooling up to 1550 °C, Metals 13 00337 i025—drainage at 1470 °C, Metals 13 00337 i026—cooling up to 1470 °C, Metals 13 00337 i027—cooling up to 870 °C, Metals 13 00337 i028—heating up to 1025 °C, Metals 13 00337 i029—heating up to 1550 °C, Metals 13 00337 i030—heating up to 1470 °C.
Metals 13 00337 g012
Figure 13. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 3), where: Metals 13 00337 i031—cooling up to 1470 °C, Metals 13 00337 i032—drainage at 1025 °C, Metals 13 00337 i033—heating up to 1025 °C, Metals 13 00337 i034—cooling up to 1025 °C, Metals 13 00337 i035—cooling at 1550 °C, Metals 13 00337 i036—heating up to 1470 °C, Metals 13 00337 i037—heating up to 1550 °C.
Figure 13. Fragment of the thermogram of quartzite, calcified at a temperature of 200 °C (Cycle 3), where: Metals 13 00337 i031—cooling up to 1470 °C, Metals 13 00337 i032—drainage at 1025 °C, Metals 13 00337 i033—heating up to 1025 °C, Metals 13 00337 i034—cooling up to 1025 °C, Metals 13 00337 i035—cooling at 1550 °C, Metals 13 00337 i036—heating up to 1470 °C, Metals 13 00337 i037—heating up to 1550 °C.
Metals 13 00337 g013
Figure 14. Fragment of the thermogram of quartzite, calcified at a temperature of 800 °C (Cycle 3), where: Metals 13 00337 i038—drainage at 800 °C, Metals 13 00337 i039—cooling up to 1470 °C, Metals 13 00337 i040—drainage at 1025 °C, Metals 13 00337 i041—heating up to 1025 °C, Metals 13 00337 i042—cooling up to 1025 °C, Metals 13 00337 i043—cooling at 1550 °C, Metals 13 00337 i044—heating up to 1470 °C, Metals 13 00337 i045—heating up to 1550 °C.
Figure 14. Fragment of the thermogram of quartzite, calcified at a temperature of 800 °C (Cycle 3), where: Metals 13 00337 i038—drainage at 800 °C, Metals 13 00337 i039—cooling up to 1470 °C, Metals 13 00337 i040—drainage at 1025 °C, Metals 13 00337 i041—heating up to 1025 °C, Metals 13 00337 i042—cooling up to 1025 °C, Metals 13 00337 i043—cooling at 1550 °C, Metals 13 00337 i044—heating up to 1470 °C, Metals 13 00337 i045—heating up to 1550 °C.
Metals 13 00337 g014
Figure 15. The enthalpy–temperature graph. Metals 13 00337 i046—Quartzite treated at a temperature of 800 °C; Metals 13 00337 i047—quartzite treated at a temperature of 200 °C.
Figure 15. The enthalpy–temperature graph. Metals 13 00337 i046—Quartzite treated at a temperature of 800 °C; Metals 13 00337 i047—quartzite treated at a temperature of 200 °C.
Metals 13 00337 g015
Table 1. Chemical composition of PKMVI-3B quartzite.
Table 1. Chemical composition of PKMVI-3B quartzite.
Chemical Composition of PKMVI-3B QuartziteContent (%)
SiO2Al2O3CaOMgOTiO2Fe2O3P2O5MnONa2OK2O
According to TU97.51.1---0.6----
Spectrometry of material dried at 200 °C96.540.9820.1890.0250.2050.930.0140.0310.1050.374
Table 2. Characteristics of elementary cell cards used in the research process.
Table 2. Characteristics of elementary cell cards used in the research process.
IndicatorsNo.
00-012-070801-071-091100-005-049001-083-218701-070-734402-002-027801-011-069501-085-062101-071-003200-018-1170
a (Å)4.99454.9134.9654.9157.124.9717.1618.49418.504
b (Å)5.4385.495.4055.4245.406---4.9915.006
Mol.
weight (g/mol)
60.0852.8760.0860.0860.0860.0860.0860.0860.0860.08
Volume (Å3)117.45118.86112.98115.79113.09360.94170.95367.062110.152215.08
Dx (g/cm3)2.5482.2162.6492.582.6472.2112.3352.1742.2702.254
c (Å)--------26.83223.845
Table 3. Average parameters and phase composition of the quartzite crystal lattice.
Table 3. Average parameters and phase composition of the quartzite crystal lattice.
Lattice ParameterTemperature (°C)
25/30 Dry200600870100014701550
davg (Å)2.814/2.8340/2.7913/2.9277/2.9796/3.0384/3.2619/
2.75742.90123.00663.05453.10483.1563.2156
Vavg3)119.1/116.55/117.47/125.86/124.06/124.04/143.65/
114.83115.41647.471653.021722.831742.691606.96
Davg (g/cm3)2.5971/2.552/2.333/2.292/2.291/2.229/2.227/
2.6012.5922.5022.26852.2662.2652.258
Mavg (g/mol)60.08/60.08/55.16/53.91/53.66/53.66/54.41/
60.0860.0860.0858.3858.6358.7958.79
Phase compositionQuartziteQuartziteQuartzite/
tridymite quartzite
Quartzite cristobalite/
tridymite quartzite
Quartzite cristobalite/
tridymite quartzite
Quartzite cristobalite/
tridymite quartzite
Quartzite cristobalite/
tridymite cristobalite
Quartzite
Table 4. Heat capacity (ΔCp) values of quartzite at the operating temperatures of melting cycles: No. 1, quartzite treated at 200 °C; No. 2, quartzite treated at 800 °C J/K.
Table 4. Heat capacity (ΔCp) values of quartzite at the operating temperatures of melting cycles: No. 1, quartzite treated at 200 °C; No. 2, quartzite treated at 800 °C J/K.
Specific Heat (ΔCp)Temperature (°C)
155014701025870102514701550147010258701025147015501470102587010251470
Quartzite No. 1 (J/K)0.0180.0140.0150.0240.0230.030.0070.0020.0100.0150.0400.0190.0150.0120.0350.0200.0220.022
Quartzite No. 2 (J/K)0.0090.0170.0370.0350.0370.0330.0180.0090.0240.0440.0500.0310.0220.0140.0200.0450.0250.029
Table 5. The enthalpy values of quartzites at the operating temperatures of melting cycles. No. 1, quartzite treated at 200 °C; No. 2, quartzite treated at 800 °C.
Table 5. The enthalpy values of quartzites at the operating temperatures of melting cycles. No. 1, quartzite treated at 200 °C; No. 2, quartzite treated at 800 °C.
EnthalpyTemperature (°C)
CoolingHeatingCoolingHeatingCoolingHeating
1550–14701470–10251025–870870–10251025–14701470–15501550–14701470–10251025–870870–10251025–14701470–15501550–14701470–10251025–870870–10251025–14701470–1550
Quartzite No. 1 (mJ/g)2263111761−57−333−14062235763234−171−369−132221871781473−364−435−1256
Quartzite No. 2 (mJ/g)1947168075−122−228−140244660457−43−322−24621749145956−116−190−2733
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Kukartsev, V.A.; Kukartsev, V.V.; Tynchenko, V.S.; Kurashkin, S.O.; Sergienko, R.B.; Tynchenko, S.V.; Panfilov, I.A.; Eremeeva, S.V.; Panfilova, T.A. Study of the Influence of the Thermal Capacity of the Lining of Acid Melting Furnaces on Their Efficiency. Metals 2023, 13, 337. https://doi.org/10.3390/met13020337

AMA Style

Kukartsev VA, Kukartsev VV, Tynchenko VS, Kurashkin SO, Sergienko RB, Tynchenko SV, Panfilov IA, Eremeeva SV, Panfilova TA. Study of the Influence of the Thermal Capacity of the Lining of Acid Melting Furnaces on Their Efficiency. Metals. 2023; 13(2):337. https://doi.org/10.3390/met13020337

Chicago/Turabian Style

Kukartsev, Viktor Alekseevich, Vladislav Viktorovich Kukartsev, Vadim Sergeevich Tynchenko, Sergei Olegovich Kurashkin, Roman Borisovich Sergienko, Sergei Vasilievich Tynchenko, Ilya Alexandrovich Panfilov, Svetlana Vitalievna Eremeeva, and Tatyana Aleksandrovna Panfilova. 2023. "Study of the Influence of the Thermal Capacity of the Lining of Acid Melting Furnaces on Their Efficiency" Metals 13, no. 2: 337. https://doi.org/10.3390/met13020337

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