By Young-jin Kim
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A. W. Wong, Proc. of ASME PVP, Vol. Y. S. S. Han, Nuclear Engineering Design 212 (2002), pp. M. Bloom, ASME PV&P Vol. 92 (1984), pp. Y. Rubinstein, Simulation and Monte Carlo Method, John Wiley & Sons. Inc. D. E. G. Price, J. of PV&P, Vol. 43 (1990), pp. L. G. P. Puls, J. of Nuclear Materials, Vol. 228 (1996), pp. 227-237 [9] O. J. F. A. S. C. Newman, Engineering and Fracture Mechanics, Vol. 15 (1981), pp. L. S. J. Y. Park, Int. J. of Modern Physics 17 (2003), pp. L. B. W. S. Lee, Trans. of KSME, Vol.
G. P. Puls, J. of Nuclear Materials, Vol. 228 (1996), pp. 227-237 [9] O. J. F. A. S. C. Newman, Engineering and Fracture Mechanics, Vol. 15 (1981), pp. L. S. J. Y. Park, Int. J. of Modern Physics 17 (2003), pp. L. B. W. S. Lee, Trans. of KSME, Vol. 28 (2004), pp. 289 [13] Hibbitt, Karlsson and Sorensen, ABAQUS User’s manual, Ver. 8 (1999) [14] A. Zahoor, Ductile Fracture Handbook, Novetech Corp. & EPRI, Vol. F. A. J. R. Duffy, ASME STP 536 (1973), pp. J.
0 Log-normal Effect of failure criteria. To verify the proposed FAD in this study, four analyses are performed. The Zahoor’s equation [14] is used to calculate the global plastic collapse stress whereas Carter’s equation [16] is used to local collapse. Leak and failure probabilities are shown in Figs. 3 and 4. Young-Jin Kim Fig. 3 Leak probability for various plastic collapse condition 41 Fig. 4 Failure probability for various plastic collapse conditions Effect of dimensional change. Physical deformations of pressure tubes, such as diametral increase, elongation, wall thickness decrease and so on, are produced as operation time elapses due to thermal creep, irradiation creep and irradiation growth.