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Volume 34 Issue 3
Jul.  2017
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LI Yang, ZHAO Qiang, ZHANG Zheng, OUYANG Xiaoping. Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide[J]. Nuclear Physics Review, 2017, 34(3): 636-640. doi: 10.11804/NuclPhysRev.34.03.636
Citation: LI Yang, ZHAO Qiang, ZHANG Zheng, OUYANG Xiaoping. Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide[J]. Nuclear Physics Review, 2017, 34(3): 636-640. doi: 10.11804/NuclPhysRev.34.03.636

Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide

doi: 10.11804/NuclPhysRev.34.03.636
Funds:  Fundamental Research Funds for Central Universities(2017MS079); National Natural Science Foundation of China(11275071, 11305061)
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  • Corresponding author: 10.11804/NuclPhysRev.34.03.636
  • Received Date: 2016-11-20
  • Rev Recd Date: 2017-05-13
  • Publish Date: 2017-07-18
  • Continuous carbon fiber reinforced silicon carbide material has the low neutron activation, low decay heat performance and tritium permeability, which are inherent performance of silicon carbide materials. It also has other advantages such as low density, small linear expansion coefficient, specific strength and specific modulus, high temperature resistance, oxidation resistance, creep resistance, thermal shock, resistance to chemical corrosion, salt fog resistance, excellent electromagnetic wave absorption properties, etc. It is an important potential candidate material in various field of nuclear engineering. In the field of nuclear fusion engineering applications, continuous carbon fiber reinforced silicon carbide as the first wall material will inevitably be bombarded by a variety of radiation particles. The radiation effect is critical to its safe use in nuclear engineering. The Monte Carlo method and the molecular dynamics method were used to study the radiation effect of protium, deuterium, tritium and helium on continuous carbon fiber reinforced silicon carbide. The SRIM and LAMMPS simulation results show that when the incident energy is 100 eV and the concentration of carbon in the continuous carbon fiber reinforced silicon carbide is about 80% ~ 85%, the sputtering yield of protium, deuterium, tritium and helium atoms have the minimum values. The kind of incident particle has a significant effect on the sputtering yield. The sputtering yield of helium atoms is larger than that of tritium atoms and deuterium atoms. There is not much difference between the sputtering yield of deuterium atoms and tritium atoms, and both the sputtering yield of deuterium atoms and tritium atoms are larger than that of protium atoms. The sputtering yield initially increases rapidly with the increase of the incident energy and then decreases gradually. The incident energy of the protium, deuterium, tritium and helium atoms has the maximum value of the sputtering yield at 200, 400, 600 and 800 eV, respectively. When the incident energy of helium atoms is 100 eV, the sputtering yield decreases while the increase of the incident angle. These results can provide a certain reference for the application of continuous carbon fiber reinforced silicon carbide materials in nuclear engineering.
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Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide

doi: 10.11804/NuclPhysRev.34.03.636
Funds:  Fundamental Research Funds for Central Universities(2017MS079); National Natural Science Foundation of China(11275071, 11305061)
    Corresponding author: 10.11804/NuclPhysRev.34.03.636

Abstract: Continuous carbon fiber reinforced silicon carbide material has the low neutron activation, low decay heat performance and tritium permeability, which are inherent performance of silicon carbide materials. It also has other advantages such as low density, small linear expansion coefficient, specific strength and specific modulus, high temperature resistance, oxidation resistance, creep resistance, thermal shock, resistance to chemical corrosion, salt fog resistance, excellent electromagnetic wave absorption properties, etc. It is an important potential candidate material in various field of nuclear engineering. In the field of nuclear fusion engineering applications, continuous carbon fiber reinforced silicon carbide as the first wall material will inevitably be bombarded by a variety of radiation particles. The radiation effect is critical to its safe use in nuclear engineering. The Monte Carlo method and the molecular dynamics method were used to study the radiation effect of protium, deuterium, tritium and helium on continuous carbon fiber reinforced silicon carbide. The SRIM and LAMMPS simulation results show that when the incident energy is 100 eV and the concentration of carbon in the continuous carbon fiber reinforced silicon carbide is about 80% ~ 85%, the sputtering yield of protium, deuterium, tritium and helium atoms have the minimum values. The kind of incident particle has a significant effect on the sputtering yield. The sputtering yield of helium atoms is larger than that of tritium atoms and deuterium atoms. There is not much difference between the sputtering yield of deuterium atoms and tritium atoms, and both the sputtering yield of deuterium atoms and tritium atoms are larger than that of protium atoms. The sputtering yield initially increases rapidly with the increase of the incident energy and then decreases gradually. The incident energy of the protium, deuterium, tritium and helium atoms has the maximum value of the sputtering yield at 200, 400, 600 and 800 eV, respectively. When the incident energy of helium atoms is 100 eV, the sputtering yield decreases while the increase of the incident angle. These results can provide a certain reference for the application of continuous carbon fiber reinforced silicon carbide materials in nuclear engineering.

LI Yang, ZHAO Qiang, ZHANG Zheng, OUYANG Xiaoping. Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide[J]. Nuclear Physics Review, 2017, 34(3): 636-640. doi: 10.11804/NuclPhysRev.34.03.636
Citation: LI Yang, ZHAO Qiang, ZHANG Zheng, OUYANG Xiaoping. Radiation Effect of Continuous Carbon Fiber Reinforced SiliconCarbide[J]. Nuclear Physics Review, 2017, 34(3): 636-640. doi: 10.11804/NuclPhysRev.34.03.636
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