Issue 36

Lj. L. Vulićević et alii, Frattura ed Integrità Strutturale, 36 (2016) 46-54; DOI: 10.3221/IGF-ESIS.36.05 47 Specimen Temperature [°C] J Ic [kN/m] K Ic [MPa  m] a c [mm] BM-NR-E 20 35.8 91.4 14.4 HAZ-NW-E 48.5 106.4 19.6 WM-NW-E 45.7 103.3 18.5 Table 1 : The values of J Ic K Ic and a c - pipe taken from service. Based on the obtained values of K Ic for the base metal (BM), heat-affected-zone (HAZ) and weld metal (WM), one can conclude that the BM has the lowest resistance to crack initiation and propagation. V ERIFICATION OF THE METHOD USING EXPERIMENTAL RESULTS OBTAINED ON STANDARD SPECIMEN he XFEM is relatively new method of numerical simulation and it has to be verified by experimental results, [3]. For this purpose the results from experimental testing and from numerical simulation using XFEM, both carried out on the standard Charpy specimen, were compared. The specimen is made of API J55 steel, the same steel as the pipe is made of. The three-point-bending test was conducted on standard Charpy specimen made from BM, since it has the lowest resistance to crack initiation and propagation. The test was conducted on high-frequency pulsator RUMUL- CRACKTRONIC at the room temperature providing relation between the crack length, a, and the number of cycles N. A finite element model of the Charpy specimen was created using the Abaqus software. Mesh was refined around the initial crack, as shown in Fig. 1. Figure 1 : Standard Charpy specimen: dimensions of the specimen and 3D model obtained using Abaqus software. The crack growth to its critical size was simulated by using Paris equation:     d d N          1.12 m a p m p C K C a p p where da/dN [m/cycles] is the fatigue crack growth, ΔK [MPa  m] the stress intensity factor range, C p and m p material parameters, which have the following value in this paper: C p =2.11  10 -15 , exponent m p = 6.166, [2]. T