Journal of Chemistry

Journal of Chemistry / 2019 / Article

Research Article | Open Access

Volume 2019 |Article ID 8793282 | 6 pages | https://doi.org/10.1155/2019/8793282

Synthesis of h-BN by the Combustion of B/KNO3/Octogen Mixture under Nitrogen Atmosphere

Academic Editor: Jae Ryang Hahn
Received31 Aug 2018
Revised18 Mar 2019
Accepted31 Mar 2019
Published22 Apr 2019

Abstract

Hexagonal boron nitride (h-BN) powders were fabricated by the combustion synthesis with B/KNO3/HMX (octogen) mixtures as reactants. X-ray diffraction (XRD) and X-ray photoelectron spectroscopy (XPS) were adopted to investigate the phase composition and the chemical composition of the products, respectively. The morphology and resistance to oxidation were studied by scanning electron microscopy (SEM) and thermogravimetry (TGA), respectively. The characterization results showed that the h-BN which was produced through this method has high purity and exhibits excellent resistance to oxidation. The purity of h-BN is improved with the increasing content of HMX in reactants with boron carbide (B4C) and boron oxide (B2O3) as main impurity, but conversely, the yields are obviously decreased. Taking the comprehensive consideration of the purity and the yields together, the optimal molar ratio of B/KNO3/HMX is 10 : 1 : 4. In addition, the experimental results indicated that the crystalline grain size grows with the increasing content of HMX. The method explored in this study does not need expensive processing facilities and equipment, which is a preferable approach for the laboratory to prepare h-BN of high purity.

1. Introduction

Hexagonal boron nitride (h-BN) is the most stable crystalline form of boron nitride with excellent thermal and chemical stability. The crystal structure of h-BN is similar with the structure of graphite which provides excellent lubricating properties. Therefore, the powder of h-BN is usually employed as a kind of lubricant [1]. h-BN ceramic has many unique properties so that it could be used as ceramic for parts of high-temperature equipment [2]. The dense shapes of h-BN formed by hot press and with boric oxide as additives can be easily machined in the desired shapes because of the platy hexagonal crystals and their orientation during the hot press consolidation [3]. Furthermore, h-BN is also widely used to improve the machinability of AlN, SiC, Si3N4, Al2O3, etc. [47]. Therefore, h-BN is an important additive of ceramics.

In industry, h-BN powder is usually obtained by the reaction of boron oxide (B2O3) or boric acid (B(OH)3) with ammonia (NH3) or urea (CO(NH2)2) under nitrogen atmosphere in the presence of activated carbon or carbon [8, 9]. The concentration of h-BN can achieve up to 98% after removing the excess boron oxide in the products through this method. h-BN could be applied as the coating material because of the excellent thermal and chemical stability, and the deposited thin film of h-BN is usually obtained through the chemical vapor deposition (CVD) [10].

Self-propagating high-temperature synthesis (SHS) or combustion synthesis (CS) is an effective way for preparing the ceramic materials [11]. SHS is also an economical and preferable approach for the preparation of ceramic as it avoids the need for expensive processing facilities and equipment. There have been many research studies concerning the fabrication of h-BN and ceramic composite containing h-BN by combustion synthesis in recent years [1214].

The present work attempted to prepare h-BN by combustion synthesis. Concerning that the chemical property of boron oxide is quite stable and the unreacted boron oxide is very difficult to be removed, boron is selected as one of the raw materials. The nitriding of boron needs nitrogen and heat; therefore, some explosives can be used as the ideal reactant. There is less oxygen and more nitrogen in cyclotetramethylene tetranitramine (HMX), and the combustion of HMX releases a lot of heat, so more h-BN is expected to be produced while less boron to be oxidized when HMX is employed as a raw material. Considering the vigorous combustion reaction between boron and potassium nitrate (KNO3), high combustion heat is generated (∼7,000 kJ·g−1), so adding proper amount of KNO3 promotes the subsequent reaction [15]. In addition, appropriate amount of KNO3 can increase the yields of resultant as reactants [16].

2. Method and Materials

2.1. Raw Materials

The amorphous boron powder from Dandong Chemical Engineering Institute Co., Ltd., (>95% in purity, 1 μm) was used without any further purification. KNO3 of analytical grade was purchased from Xuzhou Jingke Reagent Instrument Co., Ltd. Cyclotetramethylene tetranitramine (HMX) of analytical grade was obtained from Gansu Baiyin silver chemical materials plant. The pure h-BN from Aladdin Industrial Corporation, Shanghai, China (>99.9% in purity), was used for comparison with a standard h-BN sample in the study.

2.2. Synthesis

Boron reacts with KNO3 vigorously to generate potassium borate, and then the yield will be very low when the content of KNO3 in the reactants is too high. Therefore, the optimal molar ratio of boron and KNO3 in this study is set as 10 : 1. The nitrogen needed to form h-BN is mainly from HMX. One possible reaction mechanism is as follows:

In the chemical reactions, the nitrogen atoms in HMX are eventually converted to boron nitride. Theoretically, the maximum yields are achieved when the molar ratio of B/HMX is about 8 : 1 by the nitrogen conservation. In addition, boron powder is difficult to dissolve in water, and the boron powder which is not fully reacted cannot be removed in the process purification of boron nitride. In order to ensure the high purity of boron nitride, the reactant HMX overdose is required. Thus, the molar ratio of B/KNO3/HMX is set as 10 : 1 : 3, 10 : 1 : 3.5, 10 : 1 : 4, and 10 : 1 : 4.5, respectively. The reactant powders were obtained by the mixing of B/KNO3 mixture and HMX in a planetary ball mill (Focucy, F-P400) for an hour.

The reactant powders were pressed under 10 MPa for about 30 min, and the test specimens were prepared in a cylindrical shape with diameter of 8 mm and height of 20 mm. Combustion synthesis was conducted in a combustion chamber under high purity (99.99%) nitrogen of 2 MPa. The products were washed with water, and then the subsequence filtration was done after the cooling in the combustor. The insoluble products after drying were obtained as the samples to be characterized.

2.3. Characterization

The morphology of the products was observed by scanning electron microscopy (SEM, FEI Quanta 600F, USA). The phase composition was identified by X-ray diffraction (XRD, Bruker, D8 Advance, Germany); the scattering angles (two theta) is 5–60° with Cu kα radiation (λ = 1.54 Å). The chemical composition was determined by X-ray photoelectron spectroscopy (XPS, Thermo fisher, K-Alpha, USA). The resistance to oxidation of the products was tested in thermogravimetry (Mettler Toledo, TGA/DSC 1, Switzerland), each sample weighing 3 mg was placed in alumina crucible and heated from 50°C to 1500°C at a 10°C·min−1 heating rate under air atmosphere.

3. Results and Discussions

3.1. X-Ray Photoelectron Spectroscopy

The surface chemical state of the samples was valuated with XPS, and the atomic composition of B, N, C, and O in the samples is shown in Table 1.


SampleMolar ratio of B/KNO3/HMXB/%N/%C/%O/%

C110 : 1 : 340.2426.9429.962.86
C210 : 1 : 3.543.0730.1521.225.56
C310 : 1 : 443.6341.1610.624.59
C410 : 1 : 4.543.9644.848.222.98

Table 1 suggests that the B : N atomic ratio in C1 sample and C2 sample is 1.49 : 1 and 1.43, and there are also a lot of C atoms in the two samples, so there may be some boron carbide and carbon impurity in the two samples. The B : N atomic ratio is near 1 : 1 for C3 sample and C4 sample, which indicates that C3 and C4 have high purity of h-BN.

The XPS experiments show the similar spectrum for C1 sample and C2 sample and also for C3 sample and C4 sample, and only the B1s, N1s, C1s, and O ls binding energies of sample C1 and C3 are shown in this paper.

Figure 1 shows that the B1s peak could be split into a doublet, and the peaks centered at approximately 190.6 eV and 192.5 eV, which are corresponding to boron nitride and boron oxide, respectively [17, 18]. The C1s spectrum is split into three peaks, the binding energy at 283 eV is assigned to B4C, and the other two high binding energy shoulders are related to the surface contamination [19]. In addition, the N1s peak at 398 eV is also ascribed to h-BN, and the O1s peak also results from the measurement of XPS. Therefore, h-BN is the major material in C1 sample and C2 sample, and the principal impurities are B4C and B2O3.

Figure 2 shows that the B1s peak and N1s peak of C3 sample are symmetrical and could not be split into a doublet, and the binding energy at 190.6 eV and 398 eV is assigned to h-BN. In addition, C1s peak and O1s peak are originated in the surface contamination due to exposure to ambient conditions, which is similar to the results of C1s peak and O1s peak in Figure 1.

The XPS results of C1 and C3 samples also suggest that the purity of h-BN can be improved by increasing the content of HMX in the reactants. Boron reacted with potassium nitrate vigorously during the combustion process with the main products of potassium borate. Nitrogen oxides (mainly NO2 and NO) were produced during the combustion of HMX, and these nitrogen oxides could react with boron to generate h-BN. As there is oxygen in HMX, more boron oxide and boron acid will be produced if there is more HMX in the reactant which will result in the lower yields.

3.2. SEM

SEM images of the samples are shown in Figure 3.

Figure 3 indicates that all the products fabricated by combustion synthesis are thin flakes. C1 sample and C2 sample are composed of agglomerated particles with irregular small particle size, but C3 sample and C4 sample are both composed of single particle. In addition, the particle size of h-BN crystalline grain for C1 sample and C2 sample is submicron while C3 sample and C4 sample have only a few microparticles. Due to the large number of irregular particles on the surface of C1 and C2 samples, the specific surface area of C1 and C2 samples is larger than that of C3 and C4 samples, which may lead to the lower antioxidant capacity of C1 and C2 samples than that of C3 and C4 samples. From the particle shape, these irregular particles in C1 and C2 samples may not be the same substance as the single particles in C3 and C4 samples. With the increase of HMX content, the particle shapes in the sample tend to be consistent. Therefore, it could be concluded that both the purity and the size of crystalline grain increase with the increase of the content of HMX.

3.3. X-Ray Diffraction

After filtration and drying, samples of C1 and C2 are solid powder with light grey in color while white in color for C3 and C4 sample. Figures 4 and 5 show the XRD patterns of the solid products.

Figures 4 and 5 show that the main phases in the C1 sample and C2 sample are h-BN (hexagonal, PDF-34-0421) and B4C (rhombohedral, PDF-35-0798), and only h-BN for C3 sample and C4 sample are consistent with the results of XPS. Therefore, h-BN can be prepared by this method.

Similarly, h-BN and B4C are materials with high chemical and thermal stability. It is difficult to separate B4C from h-BN. Based on the results of XRD and XPS, in this case, it is evident that B4C exits as impurity when the content of HMX is low. Considering the difficulties of removing B4C, the experiment results show that it is impossible to enhance the purity by the removal of B4C, and what can be applied is only decreasing the generation of B4C through the increase of HMX. However, the yields are calculated from the obtained products and the theoretical ones, and it can be decreased obviously with the increase of HMX. Considering both the purity and the yields, the optimal molar ratio of B/KNO3/HMX is chosen as 10 : 1 : 4 in this study.

The method represented in this paper does not need expensive processing facilities and equipment, and the h-BN with high purity could be easily obtained only after the simple processing of the combustion products. In addition, the only solution used in this method is water, and the pollution of organic solvent could be avoided efficiently. Therefore, it is a preferable approach for the laboratory to prepare h-BN of high purity.

3.4. Thermogravimetry

The TGA results of C1 sample and C3 sample under air atmosphere are shown in Figure 6.

Figure 6 indicates that C1 sample begins to gain mass at about 600°C, and the mass of sample increases obviously when the temperature reaches about 1200°C. The mass of C1 sample increases slowly within the temperature range from 1200 to 1400°C, but decreases rapidly when the temperature is higher than 1400°C. There is some B4C in C1 sample which is much easier to be oxidized under higher temperature, so the mass gain is mainly due to the oxidation of B4C (R4) below 1200°C and the oxidation of h-BN from 1200 to 1400°C (R5). The oxide on the surface of the block the oxidation process of the sample, and when the temperature higher than 1400°C, the mass of sample decreases rapidly due to the evaporation of boron oxide on the C1 sample surface.

Different from samples of C1, the TGA curves of C3 samples and pure h-BN almost coincide with each other, and they begin to gain mass at about 1000°C which shows the same resistance to oxidation performance of C3 sample and the pure h-BN. This indicated that the purity of C3 sample was higher than that of C1 sample, which was also consistent with the XRD test results. Therefore, the resistance to oxidation performance can meet the requirement of the preparation of high-temperature h-BN-based ceramics. In addition, the mass loss in TGA curves ascribed the evaporation of boron oxide produced by the oxidation of B4C and h-BN.

4. Conclusions

h-BN with high purity could be prepared by combustion synthesis with B/KNO3/HMX mixture as the reactant, and the h-BN prepared in this method exhibits excellent resistance to oxidation performance. The purity of h-BN is improved but the yields are decreased obviously with the increase of HMX in the reactants, and the optimal molar ratio of B/KNO3/HMX is 10 : 1 : 4. As the method is easy and does not need expensive facilities, it is a preferable approach for the laboratory to prepare h-BN of high purity.

Data Availability

The data used to support the findings of this study are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant no. 51776175).

References

  1. B. Podgornik, T. Kosec, A. Kocijan, and Č. Donik, “Tribological behaviour and lubrication performance of hexagonal boron nitride (h-BN) as a replacement for graphite in aluminium forming,” Tribology International, vol. 81, pp. 267–275, 2015. View at: Publisher Site | Google Scholar
  2. J. Eichler and C. Lesniak, “Boron nitride (BN) and BN composites for high-temperature applications,” Journal of the European Ceramic Society, vol. 28, no. 5, pp. 1105–1109, 2008. View at: Publisher Site | Google Scholar
  3. R. W. Trice and J. W. Halloran, “Investigation of the physical and mechanical properties of hot-pressed boron nitride/oxide ceramic composites,” Journal of the American Ceramic Society, vol. 82, no. 9, pp. 2563–2565, 1999. View at: Publisher Site | Google Scholar
  4. H.-Y. Jin, W. Wang, J.-Q. Gao, G.-J. Qiao, and Z.-H. Jin, “Study of machinable AlN/BN ceramic composites,” Materials Letters, vol. 60, no. 2, pp. 190–193, 2006. View at: Publisher Site | Google Scholar
  5. Z.-H. Yang, D.-C. Jia, Y. Zhou, P.-Y. Shi, C.-B. Song, and L. Lin, “Oxidation resistance of hot-pressed SiC–BN composites,” Ceramics International, vol. 34, no. 2, pp. 317–321, 2008. View at: Publisher Site | Google Scholar
  6. S. Wang, D. Jia, Z. Yang, X. Duan, Z. Tian, and Y. Zhou, “Effect of BN content on microstructures, mechanical and dielectric properties of porous BN/Si3N4 composite ceramics prepared by gel casting,” Ceramics International, vol. 39, no. 4, pp. 4231–4237, 2013. View at: Publisher Site | Google Scholar
  7. Y. Li, G. Qiao, and Z. Jin, “Machinable Al2O3/BN composite ceramics with strong mechanical properties,” Materials Research Bulletin, vol. 37, no. 8, pp. 1401–1409, 2002. View at: Publisher Site | Google Scholar
  8. X. Gouin, P. Grange, L. Bois, P. L’Haridon, and Y. Laurent, “Characterization of the nitridation process of boric acid,” Journal of Alloys and Compounds, vol. 224, no. 1, pp. 22–28, 1995. View at: Publisher Site | Google Scholar
  9. A. Nag, K. Raidongia, K. P. S. S. Hembram, R. Datta, U. V. Waghmare, and C. N. R. Rao, “Graphene analogues of BN: novel synthesis and properties,” ACS Nano, vol. 4, no. 3, pp. 1539–1544, 2010. View at: Publisher Site | Google Scholar
  10. Y. Shi, C. Hamsen, X. Jia et al., “Synthesis of few-layer hexagonal boron nitride thin film by chemical vapor deposition,” Nano Letters, vol. 10, no. 10, pp. 4134–4139, 2010. View at: Publisher Site | Google Scholar
  11. A. G. Merzhanov, “History and recent developments in SHS,” Ceramics International, vol. 21, no. 5, pp. 371–379, 1995. View at: Publisher Site | Google Scholar
  12. H. Li, Y. Zheng, J. Han, and L. Zhou, “Microstructure, mechanical properties and thermal shock behavior of h-BN–AlN ceramic composites prepared by combustion synthesis,” Journal of Alloys and Compounds, vol. 509, no. 5, pp. 1661–1664, 2011. View at: Publisher Site | Google Scholar
  13. S.-L. Chung and Y.-H. Hsu, “Combustion synthesis of boron nitride via magnesium reduction using additives,” Ceramics International, vol. 41, no. 1, pp. 1457–1465, 2015. View at: Publisher Site | Google Scholar
  14. A. S. Mukasyan, Combustion Synthesis of Boron Nitride Ceramics: Fundamentals and Applications, Nitride Ceramics, Wiley-VCH Verlag GmbH & Co. KGaA, Hoboken, NJ, USA, 2014.
  15. X. Mei, H. Yang, X. Li, Y. Li, and Y. Cheng, “The effect of 5-amino-1H-tetrazole on the combustion performance and ignition capability of boron/potassium nitrate igniter,” Journal of Thermal Analysis and Calorimetry, vol. 120, no. 3, pp. 1749–1754, 2015. View at: Publisher Site | Google Scholar
  16. J. Sivan and Y. Haas, “Spectroscopic characterization of B/KNO3 diode-laser induced combustion,” Journal of Physical Chemistry A, vol. 117, no. 46, pp. 11808–11814, 2013. View at: Publisher Site | Google Scholar
  17. Y. Shulga and V. Loryan, “X-ray photoelectron-spectroscopy and x-ray phase-analysis of the structure of composite formed during boron powders and silicon dioxide mixture combustion in gaseous nitrogen (self-distributing high-temperature synthesis mode),” Zhurnal Neorganicheskoi Khimii, vol. 39, pp. 1096–1099, 1994. View at: Google Scholar
  18. A. R. Burke, C. R. Brown, W. C. Bowling et al., “Ignition mechanism of the titanium-boron pyrotechnic mixture,” Surface and Interface Analysis, vol. 11, no. 6-7, pp. 353–358, 1988. View at: Publisher Site | Google Scholar
  19. L. G. Jacobsohn, R. K. Schulze, M. E. H. Maia da Costa, and M. Nastasi, “X-ray photoelectron spectroscopy investigation of boron carbide films deposited by sputtering,” Surface Science, vol. 572, no. 2-3, pp. 418–424, 2004. View at: Publisher Site | Google Scholar

Copyright © 2019 Song-qi Hu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


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