1. Introduction
In the production of ferromanganese alloys, manganese ore and potentially sinter are fed to the electric furnace together with other raw materials, such as coke, flux, and quartz. Coke is required as a reducing agent for all types of ferromanganese alloys, whereas potential flux and quartz additions depend on the ore type used and the target alloy composition. The raw materials are mixed in proper weight ratios prior to entering the furnace by the use of silos, automatic transport systems, and weighing devices [
1]. The furnace process is often viewed as two distinct zones, namely, the prereduction zone and the coke bed zone. The raw materials will descend through the prereduction zone in solid state, where several reactions occur between the ascending furnace gas and the descending raw materials that have a substantial effect on the overall energy efficiency and gas emissions of the process. The ores contain higher manganese oxides (MnOx, x > 1) that will reduce to MnO in the prereduction zone according to Equations (1)–(3). These reactions are highly exothermic, where the amount of evolved heat depends on the oxygen level of the ore. The oxygen level in the ore is determined by the minerals constituting the ore, which could be MnO
2-types (O/Mn = 2) as in Comilog ore, or Mn
2O
3-types (O/Mn = 1.5) as in Nchwaning ore. This implies that a high oxygen level will minimize the electrical energy requirement of the furnace. The ore reactions further influence the energy efficiency, and gas production, by determining the occurrence of the Boudouard reaction. The Boudouard reaction (C + CO
2 = 2CO), being both carbon-consuming and highly endothermic, gains significant reaction rates at temperatures exceeding 800 °C in an industrial furnace, where its reaction extent is limited by the available CO
2. As such, the reaction temperatures and rates of the ore reduction reactions producing this CO
2 is of high importance.
Due to the large impact on energy consumption and climate gas emissions, numerous studies have been carried out to elucidate the prereduction behavior of various commercial manganese ores. The typical investigation method involves thermal treatment while monitoring the reaction rates through mass loss and/or changes in off-gas composition. The consensus of these studies is that the reactions are kinetically controlled, and the reduction behavior is highly dependent on the characteristics of the ore. This is also observed in industrial operation [
2,
3]. The rates have been observed to be influenced by parameters such as particle size, reducing agent, gas composition, heating rate, and temperature [
3,
4,
5,
6].
From laboratory-scale experiments, highly oxidized ores have been observed to produce a considerable amount of heat, elevating the temperature in the ore drastically, thus affecting the reduction rate at the specific time [
5]. As such, an increased reaction rate will lead to an increased temperature, which in turn promotes the reaction rate. The ore is mixed with the remaining raw materials in the charge mixture when it enters the furnace. While these materials do not participate in any chemical reactions at low temperatures (T < 800 °C), it is reasonable to assume that they will absorb some of the heat released from the ore reduction, and thus affect the temperature and ultimately the prereduction rates of the manganese ores. Information available on the heat transfer interaction between the raw materials during prereduction is scarce; however, some work has been published on the thermophysical properties of the various raw materials used in ferromanganese production. Ksiazek et al. [
7] showed that the thermal diffusivity of manganese ores is dependent on temperature, mineralogy and porosity, and furthermore, that quartz exhibits a higher thermal diffusivity than manganese ores.
This paper presents the investigation of the influence of inert materials on the temperature development during manganese ore prereduction by the mixing of manganese ore and quartz at various ratios.
2. Materials and Methods
The evaluated manganese ores were Comilog and Nchwaning that had been dried at 105 °C for 24 h before being crushed and sieved into size fractions of 3.33–4.00 mm and 11.2–15.0 mm. The chemical composition was determined by X-ray fluorescence, except for the MnO2, CO2, H2O and LOI content. MnO2 was determined by titration (ASTM 465-11:2017), whereas H2O and LOI were determined by thermogravimetry. Eltra (combustion-IR) was used to determine amount of carbon, which was recalculated to CO2. The amount of chemically bound moisture in the ores was estimated by heating approximately 10 g of a sample in a muffle furnace at 950 °C for 12 h. It was assumed that the potential weight loss experienced by the sample included moisture, volatiles, and potential partial decomposition of manganese oxides. The latter was determined by titration according to the aforementioned procedure.
Comilog ore is a high oxygen ore, where the majority of the manganese is present as MnO
2. It has a low content of iron and some chemically bound moisture. Nchwaning ore is a medium oxygen ore, where the %MnO
2 correlates to an O/Mn close to 1.5, i.e., that of Mn
2O
3. The chemical composition of the ores is shown in
Table 1.
Nchwaning and Comilog manganese ores, respectively, and quartz in various ratios were investigated in CO-CO
2 atmosphere under a non-isothermal temperature regime. It is assumed that quartz behaves as an inert material in the temperature range used in this investigation, where its only effect is that it absorbs the heat developed by the chemical reactions. Quartz of size 6.3–8 mm was used in all experiments. Experiments were conducted with ore (Comilog or Nchwaning) and quartz in weight ratios of 1:0, 1:1, and 1:3. An overview of the conducted experiments is shown in
Table 2.
A vertical retort tube furnace connected to a thermobalance and off-gas analyzer was used for the experiments. The sample is located in the lower parts of the crucible, placed on top of a grid. The gas inlet is at the top of the crucible, from where the gas moves through the double walls, ensuring preheating before meeting the sample from beneath. The gas ascends in the crucible and exits from the top into a gas-analyzer (NDIR). An illustration of the different components of the furnace set up is shown in
Figure 1. Two thermocouples are used in the setup, where the power control is connected to the thermocouple located in the furnace wall. A second thermocouple is placed inside the crucible, adjusted so that the hot junction is in the center of the sample. There is a known difference between the two thermocouples, as seen in
Figure 2, which is accounted for in the temperature programs, ensuring that the sample reaches the target temperature. Furthermore, the temperatures measured in the sample will reveal potential temperature changes for strongly endothermic or exothermic reactions.
Figure 2 shows the difference in sample temperature during the heating of a medium oxygen ore (Nchwaning ore) and a high oxygen ore (Comilog ore) in a CO-CO
2 atmosphere. The former shows a temperature development highly similar to that of the empty crucible, whereas the latter shows a strong positive deviation in the sample temperature during ongoing reduction.
All experiments were conducted with a heating rate of 6 °C/min from room temperature to 1000 °C in a gas atmosphere consisting of 50%CO and 50% CO2 at a total flow rate of 4 L/min. At target temperature, the atmosphere was replaced by a flow of 1 L/min of argon.
4. Discussion
Comilog ore and Nchwaning ore differ in both chemical and physical properties and as such, show dissimilar behavior during heating in reducing atmosphere. A recent study showed that the MnO
2-oxides in Comilog ore reduce in a single step to MnO at temperatures below 550 °C, where a rapid decomposition of the remaining MnO
2 to Mn
2O
3 occurs, ultimately followed by a reduction of Mn
2O
3 to MnO [
8]. The results obtained in this study are consistent with the previously reported findings for Comilog ore, as the smaller-sized particles that obtained a complete prereduction at a temperature below 550 °C showed a single-step reaction rate, whereas the larger-sized particles (11.2–15.0 mm) showed a clear shift in the reaction rate at 550 °C. Prereduction of Nchwaning ore involves the reduction of Mn
2O
3-oxides to MnO, reduction of Fe
2O
3-oxides to FeO/Fe, and decomposition of the smaller amount of carbonate present in the ore. It has been reported that the manganese and iron oxides in Nchwaning ore reduce at highly overlapping temperature ranges, initiated at temperatures exceeding 400 °C, and the decomposition of carbonate, reported to be mainly calcite, occurs at temperatures exceeding 800 °C [
8]. Previously reported findings are in accordance with the prereduction behavior observed in the present study.
Similar heating programs lead to dissimilar temperature development for Comilog and Nchwaning ores due to differences in oxygen levels and reduction rates. Comilog ore is a high oxygen ore experiencing fast reduction rates. This produces a considerable amount of heat, causing the temperature in the ore to increase. Nchwaning ore has a lower oxygen level, which, in combination with lower reduction rates, leads to a temperature increase consistent with the applied heating rate. The relation between the sample temperature and the reduction rate for Comilog ore is shown in
Figure 13. The temperature increase is initiated at a slightly higher process time compared to the reaction rate, in line with the sample temperature being a result of the reaction rate. The mixing of ore with quartz decreased the sample temperature, and thus the reduction rate of the ore, during reduction of smaller-sized (3.33–4.00 mm) Comilog ore, while larger particles appeared to be insignificantly affected. An explanation for this may be that the reduction of larger particles is more governed by diffusion, which has a low dependency on temperature. Smaller particles experience less diffusional resistance, leading to a chemical-reaction-controlled mechanism, which is more sensitive towards temperature. This would further be in line with the observations that Nchwaning ore was affected by the presence of inert material (quartz) to a low or insignificant extent in both evaluated particle sizes, as Nchwaning ore has been reported to exhibit a low porosity [
5,
9,
10], suggesting a diffusion-controlled reduction.
A mathematical description of the prereduction of manganese ores, particularly high oxygen ores, requires a relation between the reaction extent and the temperature. A complete heat balance is complex, as the temperature is affected by the thermal radiation heat, the convective heat transfer between the gas and solid phase, and the reaction heat from the ore and other raw materials. In addition, there are heat losses in the system to consider. In the current study, the contribution to the temperature development from the reaction heat and interaction between raw materials was assessed. The heat generated by the prereduction reactions can be analytically estimated by the use of Equation (4), where
is the reaction enthalpy, m is the sample mass [g],
Cp is the heat capacity [J/K·g] and Δ
T is the temperature change experienced by the sample in Kelvin.
Experimental results obtained in this study were used for the sample mass. Previously reported experimental results by Ksiazek et al. [
7] were used for the heat capacities of Comilog and Nchwaning ores. The reported heat capacities were relatively similar for Comilog and Nchwaning ores, were temperature dependent, and showed a decreasing trend with increasing temperature. The largest difference was seen at temperatures of 600–800 °C due to the decomposition of MnO
2 to Mn
2O
3 in Comilog ore, where the reported heat capacities were 0.72 J/K·g and 0.95 J/K·g for Comilog and Nchwaning, respectively, at 700 °C. The reaction enthalpies were calculated based on information found in a previous study regarding the reaction steps observed during non-isothermal reduction of Comilog and Nchwaning ores, respectively, in a CO-CO
2 atmosphere [
8]. This implies that the reduction of smaller-sized Comilog ore particles (3.33–4.00 mm) was estimated by the overall reaction of MnO
2 to MnO. For the larger-sized Comilog ore particles, the overall reduction of MnO
2 to MnO was used to evaluate development at temperatures below the exothermic peak; the exothermic peak was described by reduction of MnO
2 to Mn
2O
3, whereas the reduction after peak position was described by Mn
2O
3 to MnO. For Nchwaning ore, the reaction enthalpy was calculated for the reduction of Mn
2O
3 to MnO in a single step for both particle sizes. The temperature contribution from the remaining factors was accounted for by utilizing the temperature development recorded during the heating of quartz (assumed inert). Hence, the overall temperature development was calculated according to Equation (5), where
is the temperature development for quartz and
was calculated from Equation (4).
The calculated temperatures of the sample due to the heat of exothermic reduction are presented together with the temperatures measured by the thermocouple in
Figure 14 and
Figure 15 for sizes 3.33–4.00 mm and 11.20–15.00 mm, respectively. The calculated temperatures correlate well with the measured temperatures, showing that Nchwaning ore follows the gas temperature during reduction. Furthermore, there is a reasonable agreement between measured and calculated temperatures for Comilog ore, where the temperature increase calculated from the reaction enthalpy and reaction rates shows the same trends as the measured temperature. Nonetheless, the calculated temperature is generally lower than the measured. The magnitude of the exothermic peak was calculated to be 150 °C and 50 °C for sizes 3.33–4.00 mm and 11.2–15.0 mm, respectively. The measured peak heights were 263 °C and 151 °C, i.e., a relative increase of 75% and 205% to the calculated values. In addition to the lower peak height, the width of the exothermic peak was narrower in the calculated temperature. The calculation approach evaluates the temperature by viewing the mass as a single particle and provides an estimate for the average temperature increase of the sample. As such, it does not account for the fact that the mass consists of smaller-sized ore particles forming a cluster. A significant temperature gradient has previously been reported for Comilog ore, where a considerably higher temperature has been measured in the center of the ore cluster compared to the outer areas during prereduction [
11]. Hence, it is likely that the differences in the measured and calculated temperature originates from heat transfer effects encountered in clusters, as the temperature measurements from the laboratory-scale experiments in this study are valid for the center of the sample.
While a significant temperature increase and temperature peak are often seen in laboratory scale prereduction of high oxygen ores, it is not clear to which extent this may occur in the industrial furnace. An indication can be obtained by using Equations (4) and (5) to calculate industrial charge mixtures. The chosen mixtures were 50%Comilog-50%Nchwaning and 75%Comilog-25%Nchwaning, respectively, with metallurgical coke as reductant. Both mixtures were evaluated at a basicity ((CaO + MgO)/SiO
2) of 1. This implied that smaller amounts of limestone were added to the 75%Comilog-25%Nchwaning mixture. As an estimation for the heat capacity of coke and limestone, values for carbon and calcite retrieved from the HSC Chemistry 10 database were used. The resulting temperature development is shown in
Figure 16, where
Figure 16a shows the temperature resulting from the chemical reactions and
Figure 16b shows the overall temperature development. The calculated magnitudes of the exothermic peak were 12 °C and 17 °C for ore size 11.2–15.0 mm in 50–50 mixing ratio and 75–25 mixing ratio of Comilog and Nchwaning ores, respectively, whereas 36 °C and 55 °C were calculated for ore size 3.3–4.0 mm. These temperature increases appear to be too low to cause any local sintering; however, there might be local extreme points, potentially promoted by local uneven distribution of charge components. Furthermore, the experiments in this study were conducted at a heating rate of 6 °C/min. According to Pochart et al. [
6], the heating rates encountered in industrial operation range from 2 °C/min to 8 °C/min, where the rate decreases with increasing distance from the electrode. It has previously been shown that the magnitude of the exothermic peak is dependent on the heating rate, where a higher heating rate leads to an increased peak temperature. This may suggest that local extreme temperatures are more likely to occur closer to the electrode.