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Extra resources for Ceramic Materials for Energy Applications II
This can also be demonstrated by observing the microstructural evolution as shown in Fig. 4. The homogenous grain growth of fine SiC particles and rigid grain boundary structure developed at 1850 °C, resulting in the progress of densification and the decrease of pores on triple points. Fig. 5 shows digital images of a pellet with 40 vol% TRISO particles, sintered at 1850 °C under 20 MPa. We have successfully developed near-net (pellet) shape technique with a diameter of 8 mm and a thickness of 6mm for inert SiC matrix fuels in this study.
Dong and Y. Katoh, "Development of SiC/SiC Composites by Nano-Infiltration and Transient Eutectic (NITE) Process," Ceramic Engineering and Science Proceedings. ,311-318 (2000). 5 S. M. Dong, Y. Katoh and A. ,23, 1223-1231 (2003). 6 J. A. DiCarlo, "Microstructural Optimization of High Temperature SiC/SiC Composites," Proceedings of the 5lh International Conference on High Temperature Ceramic Matrix Composites (HTCMC5), p. 187-192, The American Ceramics Society, Ohio (2004). 7 Y. Katoh, A. Kohyama and T.
800 1000 1200 Temperature (QC) Figure 6: Fuel burnup (% FIMA) vs. temperature for HEU (Th,U)02 TRISO fueled MTR accelerated irradiation tests. 42 · Ceramic Materials for Energy Applications II SiC-Coated HTR Fuel Particle Performance Table 7: Accelerated MTR irradiation test operating conditions for HEU (Th,U)Q2 TRISO fuel. 5 xlO"9 fission gas Kr is shown for the experiments BR2-P25, FRJ2-P23. 9 xlO'7 LEU U 0 2 TRISO FUEL The nominal maximum operating conditions for the general HTR design and the HTR Modul10 employing modern LEU U0 2 TRISO fuel are listed below.