피복입자핵연료에서 증착조건이 탄화규소층의 특성에 미치는 영향
Effect of Deposition Parameters on the Property of Silicon Carbide Layer in Coated Particle Nuclear Fuels
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Tri-isotropic (TRISO) coatings on zirconia surrogate beads are deposited using a fluidized-bed vapor deposition (FB-CVD) method. The silicon carbide layer is particularly important among the coated layers because it acts as a miniature pressure vessel and a diffusion barrier to gaseous and metallic fission products in the TRISO-coated particles. In this study, we obtain a nearly stoichiometric composition in the SiC layer coated at 1400oC, 1500oC, and 1400oC with 20 vol.% methyltrichlorosilane (MTS), However, the composition of the SiC layer coated at 1300-1350oC shows a difference from the stoichiometric ratio (1:1). The density decreases remarkably with decreasing SiC deposition temperature because of the nanosized pores. The high density of the SiC layer (≥ 3.19 g/cm2) easily obtained at 1500oC and 1400oC with 20 vol.% MTS did not change at an annealing temperature of 1900°C, simulating the reactor operating temperature. The evaluation of the mechanical properties is limited because of the inaccurate values of hardness and Young’s modulus measured by the nano-indentation method.
Abstract
Tri-isotropic (TRISO) coatings on zirconia surrogate beads are deposited using a fluidized-bed vapor deposition (FB-CVD) method. The silicon carbide layer is particularly important among the coated layers because it acts as a miniature pressure vessel and a diffusion barrier to gaseous and metallic fission products in the TRISO-coated particles. In this study, we obtain a nearly stoichiometric composition in the SiC layer coated at 1400oC, 1500oC, and 1400oC with 20 vol.% methyltrichlorosilane (MTS), However, the composition of the SiC layer coated at 1300-1350oC shows a difference from the stoichiometric ratio (1:1). The density decreases remarkably with decreasing SiC deposition temperature because of the nanosized pores. The high density of the SiC layer (≥ 3.19 g/cm2) easily obtained at 1500oC and 1400oC with 20 vol.% MTS did not change at an annealing temperature of 1900°C, simulating the reactor operating temperature. The evaluation of the mechanical properties is limited because of the inaccurate values of hardness and Young’s modulus measured by the nano-indentation method.
참고문헌 (21)
- P. Hoseman, , J. Nuclear Mater, 442, pp.133~ (2013)
- J. Powers, , J. Nuclear Mater., 405, pp.74~ (2010)
- D.A. Petti, "INEIL", EXT-02-00300
- Schlichting, , Powder Metall. Int., 12, pp.196~ (1980)
- Von Muench, , J. Electrochem. Soc., 125, pp.294~ (1978)
- Stinton, D.P, , Ceram. Bull., 57, pp.568~ (1978)
- Minato, K., , J. Nuclear Mater., 149, pp.233~ (1987)
- E. Lopez-Honorato, , J. Nuclear Mater, 392, pp.219~ (2009)
- Y. J. Lee, , J. Mater. Sci., 35, pp.4519~ (2000)
- E. Lopez-Honorato, , J. Mater. Res., 23, pp.1785~ (2009)
- Zhao X, , J. Amer Ceram Soc., 94, pp.3509~ (2011)
- Chollon G, , J. Eur Cerm Soc., 27, pp.1503~ (2007)
- D. Helary, , J. Nuclear mater., 350, pp.332~ (2006)
- K.A. Appiah, , Thin Solid Films., 371 (2000)
- L. Tan, , J. Nuclear Mater., 372, pp.400~ (2008)
- D. A. Petti, , Nucl. Eng. Design., 222, pp.281~ (2003)
- S. Ray, , Appl. Phys., 99, pp.044108~ (2006)
- S. Nakashima, , Phys. Status Solidi., 39, pp.162~ (1997)
- M.D Allendorf, , J. Electrochem. Soc, 138, pp.841~ (1991)
- P. Krautwasser, , J. Amer Ceram Soc., 66, pp.424~ (1983)
- E. Lopez-Honorato, , J. Nuclear Mater., 433, pp.199~ (2013)
