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Article

Kinetic Studies on Gas-Based Reduction of Vanadium Titano-Magnetite Pellet

Department of Energy and Resources Engineering, College of Engineering, Peking University, Beijing 100871, China
*
Author to whom correspondence should be addressed.
Metals 2019, 9(1), 95; https://doi.org/10.3390/met9010095
Submission received: 5 January 2019 / Revised: 13 January 2019 / Accepted: 14 January 2019 / Published: 16 January 2019
(This article belongs to the Special Issue Ironmaking and Steelmaking)

Abstract

:
Vanadium titano-magnetite (VTM) is a significant resource in China—analysis shows that China possesses approximately 10 billion tons of VTM. In this study, we characterize VTM’s isothermal reduction mechanisms in the mixture of H2, CO, and N2 where the variables considered include reduction time, reduction temperature, gas composition, and pellet size. The kinetics of the reduction process were studied following a shrinking core model. The results indicate that the reduction degree of oxidized VTM pellets increases with increases of reduction time and reduction temperature but decreases with increasing pellet size. Moreover, we found that an increase of H2/(H2 + CO) ratio induced an increase of the reduction degree. We discuss the transformation of main Ti-bearing mineral phases, and we consider the most probable reaction mechanism. For the entire reduction process, the kinetic results confirm the existence of an early and later stages that are controlled by interface chemical reaction and diffusion, respectively. Furthermore, the results show that the diffusion-control step can be observably shortened via decreased pellet size because a thinner product layer is formed during the reduction process. Our study thus provides a valuable technical basis for industrial applications of VTM.

1. Introduction

Vanadium titano-magnetite (VTM) is a type of multi-elements-coexistent mineral that contains iron (Fe), titanium (Ti), vanadium (V), and various rare metals [1,2,3]. VTM is becoming increasingly important because of its significant value in the high-tech industries [4,5,6]. According to statistics, more than 10 billion tons VTM resources are located in China. The abundant reserves ranks China third in the world following Russia and South Africa [7,8]. The VTM with TiO2 and V2O5 is abundant in Panxi Area of China, where the amount of TiO2 and V2O5 present account for more than 90% and 80%, respectively, of the total quantity of China [9,10,11]. Hence, it is important to utilize the VTM in the Panxi Area of China as the main supply of Ti and V. Especially, the extraction of valuable elements such as vanadium in VTM has attracted the attention of many scholars [12,13]. In particular, vanadium plays a major role in many fields such as biological and medicine fields [14]. The crystalline structure of VTM is complicated because the Ti and Fe are closely associated with each other in the ore, and V is as isomorphism in the lattice of VTM [15]. The key to utilizing the resource lies in how to separate the Fe, V and Ti efficiently. The processes involved in utilizing VTM fall into two categories: blast furnace (BF) processes and non-BF processes [16,17]. The BF technology is widely recognized because it has been employed for a long time in China and Russia. However, this process does have several drawbacks. First, the continual shortage of coke resource limits development of BF technology. In addition, the introduction of limestone as a solvent in blast furnaces decreases the grade of TiO2, and the reaction of TiO2 with limestone to produce perovskite leads to almost no recycling of titanium available in VTM. Currently, much research has been conducted on the comprehensive utilization of VTM by non-BF processes, and several technological processes for the utilization of VTM have already been developed. The pre-reduction electric furnace smelting process is the most promising processes due to the high recovery rate of valuable elements and low cost [15].
Reduction is an essential procedure in the pre-reduction electric furnace smelting process. Hence, it is extremely important to investigate the reduction behavior and kinetics of VTM. In recent decades, a large number of studies have been carried out to investigate reduction behavior and kinetics of VTM. Most previous research on the reduction behavior and kinetics of VTM was mainly focused on the process that used coal as the reducing agent [12,13,18,19,20,21,22]. However, the rate of the reduction reaction is relatively slow in coal-based reduction process. In addition, with political pressure focused on environmental protection, gas-based reduction of VTM is becoming increasingly prevalent. Compared with coal-based reduction, gas-based reduction has a number of advantages, such as higher reduction degree, better processing capacity as well as less pollution [12,13,23,24,25,26]. Although a few papers have dealt with the gas-based reduction of VTM, there are two important problems in the previous research on the gas-based reduction behavior and kinetics of VTM. Firstly, many reduction experiments were based on the use of pure hydrogen (H2) or pure carbon monoxide (CO). Nevertheless, most of the reaction is between the VTM and a gas mixture of CO, H2 and N2 in the actual industrial process. Second, the previous studies did not consider the particle size of oxidized VTM pellets; this can play an important role in the reduction kinetics. Therefore, previous experiments were not carried out by simulating the actual reduction gas, and thus they are problematic for guiding the industrial application of VTM.
In this paper, the gas-based reduction kinetics of oxidized VTM pellets was examined systematically. The effects of reduction time, reduction temperature, gas composition of different H2/(H2 + CO) ratios with 25% N2, and pellet size on the VTM reduction kinetics were studied using unreacted nuclear shrinkage model. Our study is expected to provide a more valuable technical basis for industrial application of VTM.

2. Materials and Methods

2.1. Preparation of Oxidized VTM Pellets

The VTM sample used in this study was obtained from the Panzhihua and Xichang areas of Sichuan Province in China. Sample crystal phase of sample was characterized by X-ray powder diffraction (XRD; Bruker D8 ADVANCE, Germany, CuKα radiation, 40 kV, 40 mA). The XRD patterns of the VTM are shown in Figure 1a. As can be seen from Figure 1a, the main mineral phases of the VTM are magnetite (Fe3O4) and Ilmenite (FeTiO3). Elements Ti and Fe are closely associated to each other in the mineral phase.
The oxidized VTM pellets were prepared as follows. Then the VTM was fully mixed with 1 wt % binder and 8.5 wt % water and then pelletized to the diameters of 6–8 mm, 8–10 mm, 10–12 mm, 12–14 mm, and 14–16 mm in a disc pelletizer (Hong Xing Company, Shaoxing, China). Then, the VTM pellets were loaded into a quartz reactor after being dried at 110 °C for 4 h. Finally, the VTM pellets were calcined at 1350 °C for 20 min under the air conditions. The main chemical compositions are displayed in Table 1, while the XRD patterns of the oxidized VTM pellets are shown in Figure 1b. It can be seen that the main mineral phases of oxidized VTM pellets were hematite (Fe2O3) and pseudobrookite (Fe2TiO5). It can be concluded that Fe3O4 and FeTiO3 transformed to hematite Fe2O3 and Fe2TiO5 during the pre-oxidation process.

2.2. Experimental Measurements

In this study, 200 g of heated oxidized VTM pellets directly react with reducing gas in the furnace. The experimental setup is shown in Figure 2. The equipment (Beijing Hengjiu Experimental Equipment Co., Ltd., Beijing, China) consisted of a reducing gas flow control cabinet, a tube furnace, a high temperature resistant reactor made of steel alloy, a coal gas analyzer (3012H Automatic Smoke and Gas analyzer” produced in China), an electronic balance and a computer.
Firstly, 400 g corundum balls with average diameter of 1 cm were placed at the bottom of the reactor to disperse the reducing gases, and the oxidized VTM pellets were laid evenly above the corundum balls. A gasket made of silica gel was placed between the flanges to improve the air tightness of the reactor. Then the blind flange of the reactor was then closed. The inlet pipe and the exit pipe were connected with the reactor, and the reactor was filled with N2 to check the air tightness. Upon satisfactory air tightness, the reactor was suspended on the bottom of the electronic balance placed above the tube furnace. The tube furnace was turned on, and the temperature program was as the heat was applied. During the entire heating process, the reactor was filled with N2. When the temperature reached a specified level, the electronic balance and the coal gas analyzer were turned on and the data were recorded. The N2 was replaced by the reducing gas to carry out the reduction. Afterward, the reducing gas was switched for N2. Finally, the sample was taken from furnace the after cooling.
H2, CO and N2 controlled by flow-controlled cabinet were fully mixed in the mixing chamber in the reduction reaction, and the reaction pressure was 1 atm. The gas mixture entered the bottom of the reactor through the inlet pipe along the inner wall of reactor. Afterward, the reducing gas mixture met with the oxidized VTM pellets. The mass change was continuously recorded by the electronic balance and stored in the computer. It was critical to completely remove the dust and vapor in the offgas to avoid damaging the coal-gas analyzer. Thus, the offgas firstly entered into the water-wash bottle followed by a drying bottle. Later, we measured the chemical components of offgas online using the coal-gas analyzer. Finally, the off-gas was emptied. After the samples being reduced for 240 min, the VTM pellets were cooled to room temperature under an N2 atmosphere for later testing.
The reduction degree of oxidized VTM pellets can be calculated as follows [15]:
R = m ( O L ) m 0 ( O L ) = ( 0.11 w ( FeO ) 0.43 w ( TFe ) + m 1 m 2 m 1 × 0.43 w ( TFe ) ) × 100 %
In which R is reduction degree of iron, m0(OL) is the total weight of O which bonds with Fe in oxidized VTM pellets, m(OL) is the weight loss of O that bonds with Fe during reduction, w(TFe) and w(FeO) are the mass fraction of TFe and FeO respectively, in oxidized VTM pellets, m1 is the mass of the VTM pellet before reduction, and m2 is the mass of the VTM pellet in reduction process. The parameters 0.11 and 0.43 represent the oxygen demand conversion coefficients when converting FeO and Fe to Fe2O3, respectively.

2.3. Reduction Kinetics Analysis

Based on previous research [15,16], it can be concluded that the reduction of the oxidized VTM pellets proceed topochemically. Therefore, the kinetic model used to describe the iron ore reduction was the un-reacted shrinking core model. This model includes the processes of external diffusion of gaseous species, intrinsic chemical reactions, and the diffusion of gas species. Under the condition of the mixture of H2, CO and N2, the total reduction time can be calculated according to the Equation (2), which is based on the un-reacted shrinking core model. Therefore, the rate equations can be obtained as shown in Equations (3) and (4). According to Equations (3) and (4), multiple graphs can be drawn to investigate the actual rate-controlling step of the reduction process. If the process is controlled by the intrinsic chemical reaction, the plot of 1 ( 1 R ) 1 3 vs. time should be a straight line. For the diffusion of gas species controlling step, the plot of 1 2 3 R ( 1 R ) 2 3 vs. time should be a straight line. In Equation (2), Equation (3) and Equation (4), t is the total reduction time (min), k is the reduction rate constant (cm/min), r0 is characteristic initial radius of the pellet (cm), ρ0 is initial oxygen concentration in the pellet (mol/cm3), k0 is the parameter constant, c0 and cq are reduction gas concentration at granule surface and in equilibrium respectively (mol/cm3), and De is the effective diffusion coefficient (cm2/min).
t = r 0 ρ 0 k 0 ( c 0 c q ) [ 1 ( 1 R ) 1 3 ] + r 0 2 ρ 0 D e ( c 0 c q ) [ 1 2 3 R ( 1 R ) 2 3 ]
k t = 1 ( 1 R ) 1 3
k t = 1 2 3 R ( 1 R ) 2 3

2.4. Characterization

Sample crystal phase of sample was characterized by X-ray powder diffraction (XRD; Bruker D8, CuKα radiation, 40 kV, 40 mA).

3. Results and Discussion

3.1. Reduction Temperature

The reduction of VTM pellets was carried out in the temperature range of 973 K–1373 K with the intervals of 100 K. Other specific experimental conditions were controlled: The total gas flow was 5 L·min−1, the proportion of N2 was 25%, the proportion of H2 and CO was 75% (the H2/(H2 + CO) = 1/2), and the diameter of oxidized VTM pellets was 10–12 mm. The experimental results are shown in Figure 3.
It can be seen that the reduction degree of oxidized VTM pellets gradually increased with the reduction time. The reduction percentages were 49.8%, 56.0%, 71.0%, 85.0% and 93.3% at 973 K, 1073 K, 1173 K, 1273 K and 1373 K, respectively, for 80 min in H2/(H2 + CO) = 1/2 atmosphere, indicating that the reaction temperature can also strongly influence the reduction rate of oxidized VTM pellets. The reduction degree can be elevated with the increase of temperature because crystal lattice has a higher energy in higher temperature. In addition, H2 and CO have higher reduction thermodynamic potential energy as the temperature increases. Thus, the reduction temperature of oxidized VTM pellets is recommended to exceed 1273 K in actual industrial production.
Figure 4 shows the XRD patterns of the VTM pellets after the reduction process. The results indicate that Fe can be produced at 973 K–1373 K. In addition, the Ti-bearing main mineral phase changes with the increase in temperature. The phase of Fe2TiO5 disappears, and the phase of the reduction product is Fe2TiO4 at 973 K. As the temperature increases, Fe2TiO4 is reduced to FeTiO3. With the temperature further increasing to 1173 K, FeTiO3 is reduced to FeTi2O5. Therefore, the most probable reaction mechanism of the reduction process can be described in Equations (5)–(16).
3 Fe 2 O 3 +   H 2 ( g ) =   2 Fe 3 O 4 + H 2 O ( g )
Fe 3 O 4 +   H 2 ( g ) =   3 FeO + H 2 O ( g )
FeO +   H 2 ( g ) =   Fe + H 2 O ( g )
3 Fe 2 O 3 +   CO ( g ) =   2 Fe 3 O 4 + CO 2 ( g )
Fe 3 O 4 +   CO ( g ) =   3 FeO + CO 2 ( g )
FeO +   CO ( g ) =   Fe + CO 2 ( g )
Fe 2 TiO 5 +   H 2 ( g ) =   Fe 2 TiO 4 + H 2 O ( g )
Fe 2 TiO 5 +   CO ( g ) =   Fe 2 TiO 4 + CO 2 ( g )
Fe 2 TiO 4 +   H 2 ( g ) =   Fe + FeTiO 3 + H 2 O ( g )
Fe 2 TiO 4 +   CO ( g ) =   Fe + FeTiO 3 + CO 2 ( g )
2 FeTiO 3 +   H 2 ( g ) =   Fe + FeTi 2 O 5 + H 2 O ( g )
2 FeTiO 3 +   CO ( g ) =   Fe + FeTi 2 O 5 + CO 2 ( g )
On the basis of Equations (3) and (4), kinetic results of the VTM pellets are shown in Figure 5a,b. The figure clearly shows that there are two stages in the whole reduction process: an early stage and a later stage. The correlation coefficients (R2) of the straight lines are 0.982, 0.998, 0.983, 0.985 and 0.986 at the early stage. The correlation coefficient (R2) of the straight lines are 0.999, 0.998, 0.985, 0.993 and 0.997 at the later stage. Thus, the strong linear relationships indicate that the reduction processes of the early stage and the later stage are controlled by interface chemical reaction and diffusion, respectively. The values of the reduction rate constant of two stages are presented in Table 2. The reduction rate constants of both the early stage and the later stage increase with increasing temperature. This indicates that an increase in temperature can effectively improve the reduction process.
According to the Arrhenius equation, the relationship between the reaction temperature (T) and the reduction rate constant (k) can be obtained as shown in Equation (17). In Equation (17), E is the activation energy (kJ·mol−1), k0 is the frequency factor.
k = k 0 exp ( E R T )
Taking the natural logarithm of both sides in Equation (17):
ln k = E R T + ln k 0
The plot of lnk vs. 1/T in H2/(H2 + CO) = 1/2 atmosphere is shown in Figure 6a,b. The activation energies of intrinsic chemical reaction control stage and diffusion control stage can be evaluated based on the data of Figure 6 and Equation (18), and the calculated values are 41.65 kJ/mol and 92.45 kJ/mol, respectively. Therefore, the value of activation energy in intrinsic chemical reaction control stage is lower than that in diffusion control stage for gas-based reduction of oxidized VTM pellets.

3.2. Gas Composition

To investigate the effect of gas composition on the reduction of oxidized VTM pellets, the experiment was carried out under the H2/(H2 + CO) ratios of 0, 1/4, 1/3, 1/2, 2/3, 3/4, and 1. Other specific experimental conditions were controlled as follows: The reduction temperature was 1273 K, the total gas flow was 3 L·min−1, the proportion of N2 was 25%, the proportion of H2 and CO was 75%, the oxidized VTM pellets diameter was 10–12 mm. The experimental results are shown in Figure 7. For reducing under the condition of H2/(H2 + CO) = 0 for 150 min, the reduction degree of VTM pellets was only 72.6%. As the ratio of H2/(H2 + CO) increased to 1, the reduction degree of VTM pellets increases to 92.1%. This shows that the reduction degree of VTM pellets increases with the increasing H2/(H2 + CO) ratio. Previous research has confirmed that H2 has higher reduction capacity and utilization than CO at high temperature (T > 1084 K) [27,28].
Figure 8 presents the XDR patterns of the reduction VTM pellets products that were obtained after being reduced by the reduction gas with different H2/(H2 + CO) ratios at 1273 K for 240 min. The pattern indicates that when the proportion of H2/(H2 + CO) is small, the phase of Fe2TiO5 disappears, and the main phase of the reduction product is FeTiO3. The most probable reaction mechanism is given by Equations (11–14). As the ratio of H2/(H2 + CO) increases to 2, FeTiO3 is reduced to FeTi2O5. The most probable reactions are Equation (15), and Equation (16).
Figure 9a,b show the plot of 1 ( 1 R ) 1 3 vs. time and plot of 1 2 3 R ( 1 R ) 2 3 vs. time, respectively, at 1273 K in different H2/(H2 + CO) ratios. There are also both the early stage and the later stage, these are controlled by interface chemical reaction and by diffusion, respectively. The plots show that the diffusion-control step was significantly shortened as the ratio of H2/(CO + H2) increased. Therefore, the kinetic conditions of reduction can be improved at 1273 K by increasing the H2/(H2 + CO) ratio. The hydrogen-rich reduction gas is definitely beneficial to the reduction of oxidized VTM pellets in the actual industrial production.

3.3. Pellet Size

To investigate the effect of pellet size on the reduction of oxidized VTM pellets, the reduction experiments were carried out with the oxidized VTM pellets having diameters of 6–8 mm, 8–10 mm, 10–12 mm, 12–14 mm, and 14–16 mm. Other specific experimental conditions were as follows: The reduction temperature was 1273 K, the total gas flow was 5 L·min−1, the proportion of N2 was 25%, the proportion of H2 and CO was 75% (the H2/(H2 + CO) = 1/2).
As the pellet size changed from 6–8 mm to 14–16 mm, the resulting reduction degree of the oxidized VTM pellets is shown in Figure 10. It can be seen that the pellet size of oxidized VTM pellets has a strong influence on the reduction degree. The reduction degree increased with the decreasing pellet size.
Figure 11 shows the XRD patterns of the reduction VTM pellets products that were obtained at 1273 K for 240 min in H2/(H2 + CO) = 1/2 atmosphere. It can be seen that the phase of FeTiO3 can be transferred into that of Fe2TiO5 with the decrease in pellet diameter. The most probable reaction mechanism is described in Equations (11–14). Until the pellet size decreases to 10–12 mm, FeTiO3 is reduced to FeTi2O5. The most probable reactions are Equation (15), and Equation (16). With the continuous decrease of pellet size, the diffractive peaks of FeTi2O5 become weaker and the peak metallic iron getting stronger, resulting in the enhancement of reduction degree.
Figure 12a,b show the Plots of 1 ( 1 R ) 1 3 and 1 2 3 R ( 1 R ) 2 3 vs. time with different diameters of oxidized VTM pellets. It is obvious that early stage and the later stage also exists during the reduction process, these are controlled by interface chemical reaction and diffusion, respectively. It is can be seen that the pellet size has strong influence on the later stage. The thickness of the product can be decreased with decreasing pellet size during the reduction process. The diffusion degree of gas decreased quickly with the increasing thickness of product layer. This result shows that the diffusion-control step can be shortened via decreasing of the pellet size. Therefore, it is important to select the appropriate pellet size in order to optimize the reduction process. From Figure 12, the values of reaction rate constant can be obtained, and these are listed in Table 3. The results indicate that the kinetic conditions of reduction can be improved at 1273 K in H2/(H2 + CO) = 1/2 atmosphere via a decrease in the pellet size.

4. Conclusions

Gas-based reduction of oxidized VTM pellets in the mixture of H2, CO, and N2 was systematically investigated at 973 K–1373 K. The reduction degree increased with increasing reduction time, reduction temperature, and H2/(H2+CO) ratios, and decreasing pellet size. The Ti-bearing main mineral phase transformation of oxidized VTM pellets in H2/(H2 + CO) = 1/2 atmosphere is described as Fe2TiO5 → Fe2TiO4 → FeTiO3 → FeTi2O5. The Ti-bearing main mineral phase transformation of the reduction VTM pellets products at 1273 K is described as Fe2TiO5 → FeTiO3 → FeTi2O5 with the increase of H2/(H2 + CO) ratios and the decrease of pellet size. The most probable reaction mechanism is provided based on the reduction process. The kinetics of oxidized VTM pellet in the reduction process is successfully modeled as a shrinking unreacted-core. For the entire reduction process, the kinetics study indicated that there are an early stage and a later stage that are controlled by interface chemical reaction and diffusion, respectively. In addition, the diffusion-control step can be observably shortened via decreasing the pellet size because the thickness of the product layer becomes thinner in the reduction process.

Author Contributions

Conceptualization, X.W.; data curation, L.M.; formal analysis, J.C.; funding acquisition, X.W.; investigation, J.C. and W.C.; methodology, J.C. and Y.J.; resources, X.W.; software, X.W.; supervision, X.W.; visualization, J.C.; writing—original draft, J.C.; writing—review & editing, W.C.

Funding

This work was supported by the ministry of land and resources public welfare industry research project (201511062-02).

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. XRD patterns of the sample: (a) the VTM; (b) the oxidized VTM pellets.
Figure 1. XRD patterns of the sample: (a) the VTM; (b) the oxidized VTM pellets.
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Figure 2. Schematic of the experimental apparatus: 1—gas cylinder, 2—flow control cabinet, 3—gas mixing chamber, 4—reactor, 5—fever zone, 6—alundum tube, 7—corundum ball, 8—oxidized VTM pellets, 9—thermocouple, 10—tube furnace, 11—temperature controlling cabinet, 12—wash bottle, 13—drying bottle, 14—coal gas analyzer, 15—electronic balance, 16—computer.
Figure 2. Schematic of the experimental apparatus: 1—gas cylinder, 2—flow control cabinet, 3—gas mixing chamber, 4—reactor, 5—fever zone, 6—alundum tube, 7—corundum ball, 8—oxidized VTM pellets, 9—thermocouple, 10—tube furnace, 11—temperature controlling cabinet, 12—wash bottle, 13—drying bottle, 14—coal gas analyzer, 15—electronic balance, 16—computer.
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Figure 3. The reduction degree curves of oxidized VTM pellets at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Figure 3. The reduction degree curves of oxidized VTM pellets at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 4. XRD patterns of the reduction products at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Figure 4. XRD patterns of the reduction products at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 5. Plot of 1 ( 1 R ) 1 3 vs. time (a) and plot of 1 2 3 R ( 1 R ) 2 3 vs. time (b) at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Figure 5. Plot of 1 ( 1 R ) 1 3 vs. time (a) and plot of 1 2 3 R ( 1 R ) 2 3 vs. time (b) at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 6. The Arrhenius plot of reaction degree constant k vs. temperature (a) intrinsic chemical reaction control step and (b) diffusion control step at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Figure 6. The Arrhenius plot of reaction degree constant k vs. temperature (a) intrinsic chemical reaction control step and (b) diffusion control step at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 7. The reduction degree curves of oxidized VTM pellets at 1273 K with H2/(H2 + CO) ratios.
Figure 7. The reduction degree curves of oxidized VTM pellets at 1273 K with H2/(H2 + CO) ratios.
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Figure 8. XRD patterns of reduction products at 1273 K with H2/(H2 + CO) ratios.
Figure 8. XRD patterns of reduction products at 1273 K with H2/(H2 + CO) ratios.
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Figure 9. The reduction degree curves of oxidized VTM pellets at 1273 K with H2/(H2 + CO) ratios. (a) the plot of 1 ( 1 R ) 1 3 vs. time and (b) plot of 1 2 3 R ( 1 R ) 2 3 vs. time.
Figure 9. The reduction degree curves of oxidized VTM pellets at 1273 K with H2/(H2 + CO) ratios. (a) the plot of 1 ( 1 R ) 1 3 vs. time and (b) plot of 1 2 3 R ( 1 R ) 2 3 vs. time.
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Figure 10. The reduction degree curves of oxidized VTM pellets at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
Figure 10. The reduction degree curves of oxidized VTM pellets at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 11. The reduction degree curves of oxidized VTM pellets at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
Figure 11. The reduction degree curves of oxidized VTM pellets at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
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Figure 12. Plot of 1 ( 1 R ) 1 3 vs. time (a) and plot of 1 2 3 R ( 1 R ) 2 3 vs. time (b) at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
Figure 12. Plot of 1 ( 1 R ) 1 3 vs. time (a) and plot of 1 2 3 R ( 1 R ) 2 3 vs. time (b) at 1273 K with different oxidized VTM pellets diameter in H2/(H2 + CO) = 1/2 atmosphere.
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Table 1. Main chemical compositions of oxidized VTM pellets (wt %).
Table 1. Main chemical compositions of oxidized VTM pellets (wt %).
TFeFeOTiO2SiO2Al2O3MgOCaOV2O5MnOS
45.500.5913.408.426.543.281.400.540.320.037
Table 2. The values of the reduction rate constant at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Table 2. The values of the reduction rate constant at 973 K–1373 K in H2/(H2 + CO) = 1/2 atmosphere.
Temperature973 K1073 K1173 K1273 K1373 K
Intrinsic Chemical Reaction Control0.001560.002240.003020.004690.00717
Diffusion Control1.34 × 10−53.88 × 10−56.15 × 10−52.13 × 10−43.70 × 10−4
Table 3. The values of the reduction rate constant at 1273 K with different oxidized VTM pellets diameter.
Table 3. The values of the reduction rate constant at 1273 K with different oxidized VTM pellets diameter.
Pellets Diameter6–8 mm8–10 mm10–12 mm12–14 mm14–16 mm
Intrinsic Chemical Reaction Control0.006940.00570.004690.004230.00405
Diffusion Control1.66 × 10−36.35 × 10−42.12 × 10−41.58 × 10−47.64 × 10−5

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Chen, J.; Chen, W.; Mi, L.; Jiao, Y.; Wang, X. Kinetic Studies on Gas-Based Reduction of Vanadium Titano-Magnetite Pellet. Metals 2019, 9, 95. https://doi.org/10.3390/met9010095

AMA Style

Chen J, Chen W, Mi L, Jiao Y, Wang X. Kinetic Studies on Gas-Based Reduction of Vanadium Titano-Magnetite Pellet. Metals. 2019; 9(1):95. https://doi.org/10.3390/met9010095

Chicago/Turabian Style

Chen, Junwei, Weibin Chen, Liang Mi, Yang Jiao, and Xidong Wang. 2019. "Kinetic Studies on Gas-Based Reduction of Vanadium Titano-Magnetite Pellet" Metals 9, no. 1: 95. https://doi.org/10.3390/met9010095

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