An investigation on the application of a non-destructive optical strain measurement system to fracture toughness testing
作者： T R S Lima , C O D Martins , A Reguly , J F Santos
DOI: 10.1784/INSI.2010.52.5.255
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sci-hub.se 参考文章(14)
Masanori KIKUCHI, Kazunori YANO, Analysis of the HRR Stress Field at the Three-Dimensional Crack TIP : Analysis of CT and CCT Specimens JSME international journal. Series 1, solid mechanics, strenght of materials. ,vol. 33, pp. 179- 185 ,(1990) , 10.1299/JSMEA1988.33.2_179
T.L. Anderson, Fracture Mechanics : Fundamentals and Applications NASA STI/Recon Technical Report A. ,vol. 92, pp. 40200- ,(2017) , 10.1201/9781315370293
David Broek, The practical use of fracture mechanics ,(1988)
A Haddi, D Weichert, None, Elastic-plastic J-integral in inhomogeneous materials Computational Materials Science. ,vol. 8, pp. 251- 260 ,(1997) , 10.1016/S0927-0256(97)00008-6
Y.P. Lei, Y.W. Shi, H. Murakawa, Y. Luo, The effect of mechanical heterogeneity and limit load of a weld joint with longitudinal weld crack on the J-integral and failure assessment curve International Journal of Pressure Vessels and Piping. ,vol. 75, pp. 625- 632 ,(1998) , 10.1016/S0308-0161(98)00067-2
C. A. Popelar, M. F. Kanninen, H. Saunders, Advanced Fracture Mechanics ,(1985)
J. Neves, A. Loureiro, Fracture toughness of welds—effect of brittle zones and strength mismatch Journal of Materials Processing Technology. ,vol. 153, pp. 537- 543 ,(2004) , 10.1016/J.JMATPROTEC.2004.04.120
G.B. May, A.S. Kobayashi, Plane stress stable crack growth and J-integral/HRR field International Journal of Solids and Structures. ,vol. 32, pp. 857- 881 ,(1995) , 10.1016/0020-7683(94)00165-S
K.S. Zhang, Analysis of deformation and fracture for cracked specimen of ductile steel Engineering Fracture Mechanics. ,vol. 53, pp. 625- 632 ,(1996) , 10.1016/0013-7944(95)00112-3
J. R. Rice, A Path Independent Integral and the Approximate Analysis of Strain Concentration by Notches and Cracks Journal of Applied Mechanics. ,vol. 35, pp. 379- 386 ,(1968) , 10.1115/1.3601206