{"title":"开发 Cf/C-UHTC 复合材料并研究其在高速高焓空气等离子体流中的抗氧化性和抗烧蚀性","authors":"A.N. Astapov , V.A. Pogodin , I.V. Sukmanov , B.E. Zhestkov , M.V. Prokofiev","doi":"10.1016/j.ijlmm.2024.02.003","DOIUrl":null,"url":null,"abstract":"<div><p>This article contains the results of research on the development of a C<sub>f</sub>/C-UHTC carbon fabric composite based on a viscose precursor and a combined matrix consisting of partially sintered ceramics in a system consisting of HfC–HfB<sub>2</sub>–NbC–NbB<sub>2</sub>–TiC–TiB<sub>2</sub>–B<sub>4</sub>C–SiC, amorphous carbon, and pyrocarbon. The SiC fraction does not exceed 8.5–9.0 wt%. In its initial state, the composite has open porosity, with apparent and true densities of 18–22%, 2.25–2.29 g/cm<sup>3</sup> and 2.79–2.91 g/cm<sup>3</sup>, respectively. The bending strength and the elasticity modulus are 27.8 ± 0.7 MPa and 7.8 ± 0.2 GPa, respectively, and the fracture strain is 0.85 ± 0.05%. The tests for resistance to oxidation and ablation were carried out in a gas dynamic flow regime and non-equilibrium air plasma heating at flow rates of 4.5–4.8 km/s and breaking enthalpy of 45–50 MJ/kg. Heating was performed in the temperature range <em>T</em><sub><em>w</em></sub> = 1400–2700 °C at the critical point on the front surface of the samples. The average linear ablation rate and mass loss rate of the composite are 6.3 ± 0.3 μm/s and 6.22 ± 0.44 mg/s. The estimated value of the conductivity factor is 0.280–0.285 W/(m K). The performance ability of the composite arises from the formation and evolution of a passivating heterogeneous oxide film consisting mainly of titanium niobate Ti<sub>2</sub>Nb<sub>10</sub>O<sub>29</sub>, mixed solutions of Hf<sub>1</sub><sub>−</sub><sub>x</sub>Ti<sub>x</sub>O<sub>2</sub>, (Ti<sub>1</sub><sub>−</sub><sub>x</sub>Hf<sub>x</sub>)<sub>1</sub><sub>−</sub><sub>y</sub>Nb<sub>y</sub>O<sub>z</sub> and (Ti<sub>1</sub><sub>−</sub><sub>x</sub>Hf<sub>x</sub>)NbO<sub>4</sub> with broad homogeneity ranges, and also encapsulated carbide and boride particles. It is shown that the oxidation resistance of the composite increases as a result of the transition through a number of phases into a liquid state as the working temperature increases.</p></div>","PeriodicalId":52306,"journal":{"name":"International Journal of Lightweight Materials and Manufacture","volume":"7 3","pages":"Pages 362-377"},"PeriodicalIF":0.0000,"publicationDate":"2024-02-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2588840424000131/pdfft?md5=b526ae46620093450c69195fab788bd3&pid=1-s2.0-S2588840424000131-main.pdf","citationCount":"0","resultStr":"{\"title\":\"Development of Cf/C-UHTC composite and study of its resistance to oxidation and ablation in high-speed high-enthalpy air plasma flow\",\"authors\":\"A.N. Astapov , V.A. Pogodin , I.V. Sukmanov , B.E. Zhestkov , M.V. Prokofiev\",\"doi\":\"10.1016/j.ijlmm.2024.02.003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>This article contains the results of research on the development of a C<sub>f</sub>/C-UHTC carbon fabric composite based on a viscose precursor and a combined matrix consisting of partially sintered ceramics in a system consisting of HfC–HfB<sub>2</sub>–NbC–NbB<sub>2</sub>–TiC–TiB<sub>2</sub>–B<sub>4</sub>C–SiC, amorphous carbon, and pyrocarbon. The SiC fraction does not exceed 8.5–9.0 wt%. In its initial state, the composite has open porosity, with apparent and true densities of 18–22%, 2.25–2.29 g/cm<sup>3</sup> and 2.79–2.91 g/cm<sup>3</sup>, respectively. The bending strength and the elasticity modulus are 27.8 ± 0.7 MPa and 7.8 ± 0.2 GPa, respectively, and the fracture strain is 0.85 ± 0.05%. The tests for resistance to oxidation and ablation were carried out in a gas dynamic flow regime and non-equilibrium air plasma heating at flow rates of 4.5–4.8 km/s and breaking enthalpy of 45–50 MJ/kg. Heating was performed in the temperature range <em>T</em><sub><em>w</em></sub> = 1400–2700 °C at the critical point on the front surface of the samples. The average linear ablation rate and mass loss rate of the composite are 6.3 ± 0.3 μm/s and 6.22 ± 0.44 mg/s. The estimated value of the conductivity factor is 0.280–0.285 W/(m K). The performance ability of the composite arises from the formation and evolution of a passivating heterogeneous oxide film consisting mainly of titanium niobate Ti<sub>2</sub>Nb<sub>10</sub>O<sub>29</sub>, mixed solutions of Hf<sub>1</sub><sub>−</sub><sub>x</sub>Ti<sub>x</sub>O<sub>2</sub>, (Ti<sub>1</sub><sub>−</sub><sub>x</sub>Hf<sub>x</sub>)<sub>1</sub><sub>−</sub><sub>y</sub>Nb<sub>y</sub>O<sub>z</sub> and (Ti<sub>1</sub><sub>−</sub><sub>x</sub>Hf<sub>x</sub>)NbO<sub>4</sub> with broad homogeneity ranges, and also encapsulated carbide and boride particles. It is shown that the oxidation resistance of the composite increases as a result of the transition through a number of phases into a liquid state as the working temperature increases.</p></div>\",\"PeriodicalId\":52306,\"journal\":{\"name\":\"International Journal of Lightweight Materials and Manufacture\",\"volume\":\"7 3\",\"pages\":\"Pages 362-377\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-02-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S2588840424000131/pdfft?md5=b526ae46620093450c69195fab788bd3&pid=1-s2.0-S2588840424000131-main.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Lightweight Materials and Manufacture\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2588840424000131\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Engineering\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Lightweight Materials and Manufacture","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2588840424000131","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Engineering","Score":null,"Total":0}
Development of Cf/C-UHTC composite and study of its resistance to oxidation and ablation in high-speed high-enthalpy air plasma flow
This article contains the results of research on the development of a Cf/C-UHTC carbon fabric composite based on a viscose precursor and a combined matrix consisting of partially sintered ceramics in a system consisting of HfC–HfB2–NbC–NbB2–TiC–TiB2–B4C–SiC, amorphous carbon, and pyrocarbon. The SiC fraction does not exceed 8.5–9.0 wt%. In its initial state, the composite has open porosity, with apparent and true densities of 18–22%, 2.25–2.29 g/cm3 and 2.79–2.91 g/cm3, respectively. The bending strength and the elasticity modulus are 27.8 ± 0.7 MPa and 7.8 ± 0.2 GPa, respectively, and the fracture strain is 0.85 ± 0.05%. The tests for resistance to oxidation and ablation were carried out in a gas dynamic flow regime and non-equilibrium air plasma heating at flow rates of 4.5–4.8 km/s and breaking enthalpy of 45–50 MJ/kg. Heating was performed in the temperature range Tw = 1400–2700 °C at the critical point on the front surface of the samples. The average linear ablation rate and mass loss rate of the composite are 6.3 ± 0.3 μm/s and 6.22 ± 0.44 mg/s. The estimated value of the conductivity factor is 0.280–0.285 W/(m K). The performance ability of the composite arises from the formation and evolution of a passivating heterogeneous oxide film consisting mainly of titanium niobate Ti2Nb10O29, mixed solutions of Hf1−xTixO2, (Ti1−xHfx)1−yNbyOz and (Ti1−xHfx)NbO4 with broad homogeneity ranges, and also encapsulated carbide and boride particles. It is shown that the oxidation resistance of the composite increases as a result of the transition through a number of phases into a liquid state as the working temperature increases.