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Preparation of HfC(x)N(1−x) Nanoparticles Derived from a Multifunction Precursor with Hf-O and Hf-N Bonds

HfC(x)N(1−x) nanoparticles were synthesized using the urea-glass route, employing hafnium chloride, urea, and methanol as raw materials. The synthesis process, polymer-to-ceramic conversion, microstructure, and phase evolution of HfC(x)N(1−x)/C nanoparticles were thoroughly investigated across a wid...

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Detalles Bibliográficos
Autores principales: Zeng, Guang, Xu, Ping, Zeng, Chen, Huang, Qizhong, Su, Zhean
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10303935/
https://www.ncbi.nlm.nih.gov/pubmed/37374609
http://dx.doi.org/10.3390/ma16124426
Descripción
Sumario:HfC(x)N(1−x) nanoparticles were synthesized using the urea-glass route, employing hafnium chloride, urea, and methanol as raw materials. The synthesis process, polymer-to-ceramic conversion, microstructure, and phase evolution of HfC(x)N(1−x)/C nanoparticles were thoroughly investigated across a wide range of molar ratios between the nitrogen source and the hafnium source. Upon annealing at 1600 °C, all precursors demonstrated remarkable translatability to HfC(x)N(1−x) ceramics. Under high nitrogen source ratios, the precursor exhibited complete transformation into HfC(x)N(1−x) nanoparticles at 1200 °C, with no observed presence of oxidation phases. In comparison to HfO(2), the carbothermal reaction of HfN with C significantly reduced the preparation temperature required for HfC. By increasing the urea content in the precursor, the carbon content of the pyrolyzed products increased, leading to a substantial decrease in the electrical conductivity of HfC(x)N(1−x)/C nanoparticle powders. Notably, as the urea content in the precursor increased, a significant decrease in average electrical conductivity values was observed for the R4-1600, R8-1600, R12-1600, and R16-1600 nanoparticles measured at a pressure of 18 MPa, yielding values of 225.5, 59.1, 44.8, and 46.0 S·cm(−1), respectively.