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Article

Mechanism of Microwave Activation on Molybdenite

School of Metallurgical Engineering, Xi’an University of Architecture and Technology, Xi’an 710055, China
*
Author to whom correspondence should be addressed.
Materials 2021, 14(19), 5486; https://doi.org/10.3390/ma14195486
Submission received: 23 July 2021 / Revised: 16 September 2021 / Accepted: 18 September 2021 / Published: 22 September 2021

Abstract

:
The effect of microwave activation on the properties of oxidation roasting for molybdenite was investigated under the protection of inert gas, and the specific surface area, the oxidation properties, lattice constant, microstructure, and shape of molybdenite were analyzed and characterized by a laser particle size analyzer, thermogravimetry (TG), X-ray diffractometry (XRD) and scanning electron microscopy (SEM). The results show that microwave activation could effectively reduce the residual amount of sulfur in the molybdenum calcine and decrease the average particle size of molybdenite while increasing the specific surface area of molybdenite. On increasing the microwave activation power, the crystal cell volume and grain size of MoS2 reduced, and the microstrain increased slightly. At the same time, the surface shape of molybdenite became looser, but the layered structure is not changed. In addition, the oxidation property changed significantly; microwave activation promoted the oxidation reaction of molybdenite above 538 °C, and the rate of weight loss increased from 6.177% to 7.718% at 620 °C.

1. Introduction

Molybdenum, low alloy-based material of molybdenum and molybdenum compounds, is widely used in metallurgical, chemical, and nuclear applications, for building materials, metal pressure machining, machinery, military, and other industries [1,2,3]. Molybdenum is a refractory rare metal with high strength and corrosion resistance. At present, there are only four mineral sources for molybdenum with application value, i.e., molybdenite (MoS2), CaMoO4, Fe[MoO4]3∙7H2O, and PbMoO4. Most molybdenum in the world exists in the form of molybdenite (MoS2), it is the main raw material for extracting molybdenum. Molybdenite is typically used as a catalyst, lubricant, and raw material for the production of electronic components. It is soft, has a metallic luster, and like graphite, it is a thin plate or squamous crystal. In industry, oxidative decomposition along with the ammonia leaching process is generally used for treating molybdenite. The oxidative decomposition process mainly includes oxidizing, roasting, decomposition, and hydro-decomposition. Oxidizing-roasting-decomposition is the main technological process for disposing of molybdenite due to its advantage of low consumption and low cost [4,5,6,7,8], while hydro-decomposition requires expensive equipment [9]. Byung-Su Kim et al. [10] studied the effects of temperature and particle size on oxidative roasting of low-grade molybdenite concentrate. A, M, Abdel-Rehim [11] studied the thermal analysis of oxidative roasting of Egyptian molybdenite. Ebrahimi Kahrizsangi et al. [12] studied thermal analysis of Molybdenite oxidation and demonstrated its oxidation begins at 350 °C. Gan et al. [13] studied the reactivity of low-grade molybdenum concentrates during oxidative roasting. Chen et al. [14] studied and identified the optimum conditions for the extraction of molybdenum from low-grade molybdenum concentrates by calcium-based roasting and acid leaching processes. In addition, the more chemically stable is the sulfide, the more difficult is the extraction. Thus, either drastic reaction conditions are required or the chemical stability of sulfides has to be modified by a suitable pre-leaching treatment. Hu et al. [15] studied structural changes in mechanically activated molybdenite and the effect of mechanical activation on molybdenite. The result shows that mechanically activated molybdenite is easier to be oxidized than unactivated molybdenite. However, the process of mechanical activation is complex and it consumes significantly high energy. Therefore, it is necessary to develop a low energy consuming and high-efficiency method to activate molybdenite.
Microwave heating, as a special heating method, is on the basis of conductivity of the material, magnetic permeability, and dielectric constant, which can generate heat effectively throughout the material [16]. Microwave heating is widely used in many fields due to its high heating rates, reduced processing time, and significant energy saving [17]. The selective heating and non-thermal effect can effectively change the structure and properties of the minerals. Iron ore can be reduced by carbothermal reduction in microwave field to obtain metallic iron [18,19]. Mohsen Farahat et al. [20] showed that the magnetic properties of molybdenite remained unchanged after microwave treatment. Guo et al. [21] studied the characteristics of the microwave drying and dehydrating process for molybdenum, and claimed that the energy required was twice as much as that required for conventional drying.
In this article, the structure and properties of non-activated molybdenite, as well as microwave, activated molybdenite, were investigated for the first time to reveal the mechanism of microwave activation on molybdenite and the effect of microwave activation on the properties of oxidation roasting.

2. Experiment Procedure

2.1. Materials

Molybdenite was obtained from the Jinduicheng Molybdenum Co., Ltd. (Xi’an, China), and its chemical composition is shown in Table 1. Molybdenite (mineral) has 52.21 wt.% of molybdenum, and the main gangues are SiO2, CaO, and MgO. The particle size analysis and XRD patterns of molybdenite are shown in Table 2 and Figure 1, respectively. It can be seen from Figure 1 that molybdenum mainly exists in the form of MoS2.

2.2. Preparation of Microwave Activated Molybdenite

The preparation of microwave-activated molybdenite was carried out by the microwave chemical synthesizer (MKX-R1C1C, Qingdao Maikewei Microwave Innovation Technology Co., Ltd., Qingdao, China). First, 30 g of molybdenite was loaded into a quartz tube 35 mm in diameter and 800 mm in length. N2 was passed through the quartz tube at a flow rate of 0.5 L/min for 5 min before starting the microwave oven. Then, N2 was passed through the quartz tube at a rate of 1 L/min after opening the microwave oven. The molybdenite was radiated with microwaves for 6 min at 450 W, 550 W, and 650 W of power, respectively (a unique sample for each series of power, the repeatability of the process has been verified). Finally, N2 flow was stopped until the temperature dropped below 100 °C, and the microwave-activated molybdenite was taken out and tested. The microwave-activated molybdenite samples were named P-450, P-550, and P-650, respectively.

2.3. Oxidization Roasting Experiment and Determination of Sulfur Content

The oxidization roasting of the microwave activated molybdenite and nonactivated molybdenite (P-0) were carried out in ceramic crucibles, heated in a high-temperature resistance furnace (SK-2-12, Tianjin Intermediate Belt Experiment Electric Stove Co., Ltd., Tianjin, China) under air current at a temperature of 600 °C for 2 h and after the removal of sulfur dioxide gas, oxidized molybdenite was obtained. The calcined molybdenum was removed after roasting and tested. Being on the basis of the microwave power used in the previous steps, the molybdenum calcine samples were named M-0, M-450, M-550, and M-650, respectively.

2.4. Analysis and Characterization

The sulfur content in the molybdenum calcine samples was measured by a high-frequency infrared carbon and sulfur analyzer (JS-HW2000A, Nanjing Jinshi Analysis Instrument Factory, Nanjing, China).
Particle size was analyzed by a laser particle size analyzer (Ls-800, Zhuhai OMEC Instruments Co., Ltd., Zhuhai, China), with 95% ethanol as the dispersant, and the specific surface area (SG) of the samples was calculated from the particle size distribution.
The X-ray diffraction patterns of the microwave-activated molybdenite and nonactivated molybdenite were recorded by an X-ray diffractometer (Rigaku International Corporation, Tokyo, Japan) with Cu kα radiation at 40 kV and 20 mA. Then diffraction peaks (002) and (008) were chosen for the different molybdenites, the corresponding lattice constants, average grain size (D), and microstrain (ε) were calculated by the method of Hall, the Gaussian function model, and the Jade software (Livermore, CA, USA), respectively.
The microstructures of the samples were investigated by a scanning electron microscope (JSM-5600LV, JEOL, Tokyo, Japan).
The thermal analysis study of the samples was carried out with a comprehensive thermal analyzer (STA409PC, NETZSCH, Bavaria, Germany), with 5 mg of sample; temperatures ranging from ambient to 700 °C, in air, at a heating rate of 10 °C/min.

3. Results and Discussion

3.1. Sulfur Content of Molybdenum Calcine Samples

The sulfur contents of the molybdenum calcine samples are shown in Figure 2. M-450, M-550, and M-650 had sulfur content lower than that in M-0, and as microwave activation power increased, the sulfur content in the molybdenum calcine samples decreased significantly. This can be attributed to molybdenite being oxidized more fully after microwave activation.

3.2. Specific Surface Area (SV)

The relationship between specific surface area and power is shown in Figure 3.
Figure 3 shows that microwave activation reduced the average particle diameter and increased the specific surface area of molybdenite, which can be explained by the following three reasons:
(1)
In the microwave field, MoS2 and gangue have different heating rates and they can be heated up to different temperatures because of their different abilities to absorb microwaves. The obvious temperature difference between them can produce thermal stress, which can generate cracks when thermal stress reaches a certain level. The generation of cracks can effectively promote the monomer dissociation of MoS2, thereby increasing the specific surface area of the molybdenite [22].
(2)
Due to the uneven distribution of the molybdenite components, the dispersed distribution of MoS2 can also lead to an obvious selective heating phenomenon, making internal cracks and increasing the specific surface area of the molybdenite [23].
(3)
According to the isothermal gas equation, P·V = n·R·T, the higher is the temperature, the greater is the pressure of the gas. Microwave heating occurs from the inside out, so the internal gas pressure is greater than that outside. The internal gas tends to spread outward and promote the generation of cracks. In addition, the higher the microwave power, the more obvious the change is. This can be attributed to the microwave field, the material absorbing energy can be expressed by Equation (1) [24], ε0 is the permittivity of vacuum, ε0 = 8.85 × 10−12 F/m; where ε is the loss factor, F/m; tgδ is the loss of dielectric tangent; E is the electric field intensity of internal material, V/m; and V is the volume of material, m3. It can be seen that if f and V remain unchanged, increasing the microwave power can strengthen the capacity of the material to absorb the microwave directly. The selective heating effect will be more obvious, and the specific surface area of molybdenite will gradually increase.
W = 2 π f ε 0 ε t g δ E 2 V

3.3. Analysis of XRD and SEM

X-ray diffraction peaks (002) and (008) for different molybdenite specimens are shown in Figure 4a,b. It is evident that with the increase of microwave radiation power, peaks (002) and (008) of molybdenite surrounded area gradually decreases, and the width of the half peak gradually increases. Therefore, the grain size of the molybdenite decreases after microwave activation according to the Scherrer formula.
The lattice constant, average grain size (D), and microstrain (ε) of unactivated molybdenite, as well as microwave, activated molybdenite are shown in Table 3. It can be seen that MoS2 is distorted after the treatment of microwave activation. With the increase of microwave power, the values of lattice constants a, b, and c, and D decreased gradually, while the value of ε increased slightly. The dissociation effect and activation effect of the microwave on the molybdenite is illustrated [25].
The microwave activation had only a small effect on the structure of the molybdenite, which may be related to the special structure of molybdenite and its change in shape during microwave activation. The SEM analysis of molybdenite in Figure 5a–d shows that the surface shape of molybdenite becomes looser after microwave activation. This indicates that microwave activation can improve the thermodynamics and kinetics conditions of the oxidation roasting process of molybdenite, thereby decreasing the sulfur content of the product. However, microwave activation cannot change the inherent lamellar structure of the molybdenite. This can be attributed to the hexagonal plate of molybdenite; thus, it shows excellent cleavage. Layers are connected by very strong van der Waals force; when subjected to the external force, each layer can slide along the cleavage easily, which results in reduced lattice deformation and maintains the inherent lamellar structure [26].

3.4. Analysis of the TG Curve

The TG curves for nonactivated and microwave-activated molybdenite samples are presented in Figure 6. It shows that the weight loss of all molybdenite samples starts at 440 °C. In addition, different samples have different mass loss ratios above 538 °C. The result suggests that microwave activation only promotes the oxidation reaction of molybdenite above 538 °C. The mass loss ratio at 620 °C for different molybdenite samples in the TG curves is also presented in Table 4, which can be explained by the following:
(1)
The increase in the specific surface area and the value of ε with the increased power of microwave add an effective reaction area between the molybdenite and oxygen.
(2)
In the presence of the microwave, both polar and nonpolar molecules are polarized, which results in the exchange between microwave energy stored in the molecule and the average kinetic free energy of the molecule, reducing the activation energy and promoting the reaction process.
(3)
The frequency of the microwave is very high, which may be close to the natural vibration frequency of the molecule; this may cause vibrations caused by microwave fracture of different chemical bonds, thereby promoting selective reaction activity [27,28,29].

4. Conclusions

(1)
Microwave activation can effectively reduce the sulfur content of molybdenum calcine samples obtained from molybdenite. The reason is that microwave activation can improve the thermodynamic and kinetic conditions of the molybdenite oxidation roasting process and oxidize molybdenite more thoroughly than before treatment.
(2)
After microwave activation, the specific surface area of molybdenite increased. The structural parameters and material properties of MoS2, the main component of molybdenite, were changed by microwave activation.
(3)
With the extension of microwave activated power, the crystal cell volume and grain size of MoS2 reduced, the microstrain increased slightly, and morphologic features of the surface of molybdenite became looser.
(4)
Microwave activation significantly changed the oxidation characteristics of molybdenite and promoted its oxidation reaction above 538 °C. The weight loss rate increased from 6.177% to 7.718% at 620 °C. The extension of activation time improved the conversion of molybdenite and accelerated the reaction rate of molybdenite.

Author Contributions

Conceptualization, S.Y. and T.Z.; methodology, S.L. and H.S.; writing—original draft preparation, S.Y. and T.Z.; writing—review and editing, T.Z. and H.S; supervision, S.Y. and S.L.; All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the “Project on new ferromolybdenum smelting thermodynamics and slag systematization (20200338)”.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data presented in this study cannot be shared at this time as the data also forms part of an ongoing study.

Acknowledgments

The authors were appreciated for the precious comments and suggestions of the editors and reviewers.

Conflicts of Interest

The authors declare no conflict of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

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Figure 1. XRD pattern of the molybdenite.
Figure 1. XRD pattern of the molybdenite.
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Figure 2. Sulfur content of the different samples.
Figure 2. Sulfur content of the different samples.
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Figure 3. Relationship between specific surface area and power.
Figure 3. Relationship between specific surface area and power.
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Figure 4. Peaks of XRD patterns for different molybdenite samples (a) (002) peak and (b) (008) peak. (1) P-0; (2) P-450; (3) P-550; (4) P-650.
Figure 4. Peaks of XRD patterns for different molybdenite samples (a) (002) peak and (b) (008) peak. (1) P-0; (2) P-450; (3) P-550; (4) P-650.
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Figure 5. SEM images of molybdenite (a) t = 0 min; (b) t = 3 min; (c) t = 6 min; (d) t = 9 min.
Figure 5. SEM images of molybdenite (a) t = 0 min; (b) t = 3 min; (c) t = 6 min; (d) t = 9 min.
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Figure 6. TG curves of the different samples.
Figure 6. TG curves of the different samples.
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Table 1. Chemical composition of molybdenite (%).
Table 1. Chemical composition of molybdenite (%).
MoSCuPbWO3BiCKFeSiO2CaOMgO
52.2134.830.110.090.100.050.400.090.335.201.704.89
Table 2. Particle size distribution of molybdenite.
Table 2. Particle size distribution of molybdenite.
Mass Fraction/%
>0.044 mm0.036~0.044 mm<0.036 mm
0.148.6691.2
Table 3. Lattice constant, average grain size (D), and microstrain (ε) of nonactivated and microwave activated molybdenite.
Table 3. Lattice constant, average grain size (D), and microstrain (ε) of nonactivated and microwave activated molybdenite.
Systema = b/
nm
c/
nm
α = β/
(°)
γ/
(°)
Lattice Volume/
nm3
D/
nm
ε/
%
P-00.316591.23142901200.1068986.90
P-4500.316461.23156901200.1068179.10.104
P-5500.316441.23055901200.1067274.00.119
P-6500.316401.22947901200.1066272.40.148
Table 4. The mass loss ratio at 620 °C for different molybdenites in the TG curves.
Table 4. The mass loss ratio at 620 °C for different molybdenites in the TG curves.
SamplesP-0P-450P-550P-650
Mass loss ratio/%6.1776.8817.3867.718
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Yang, S.; Zhang, T.; Liu, S.; Sun, H. Mechanism of Microwave Activation on Molybdenite. Materials 2021, 14, 5486. https://doi.org/10.3390/ma14195486

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Yang S, Zhang T, Liu S, Sun H. Mechanism of Microwave Activation on Molybdenite. Materials. 2021; 14(19):5486. https://doi.org/10.3390/ma14195486

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Yang, Shuangping, Tiantian Zhang, Shouman Liu, and Haixing Sun. 2021. "Mechanism of Microwave Activation on Molybdenite" Materials 14, no. 19: 5486. https://doi.org/10.3390/ma14195486

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