KI–T estimation for embedded flaws in pipes – Part II: Circumferentially oriented cracks
Introduction
Cylindrical structures, e.g., oil and gas pipelines and pressure vessels, contain potentially crack-like defects caused by, e.g., lack of fusion during the welding procedure. These cracks may grow to critical sizes sufficient to cause catastrophic structural failure during the operation of the pipelines and pressure vessels. Recent research work reported by SINTEF shows that embedded circumferential flaws in the wall of a pipe can, in certain circumstances, impose a more critical threat to the safety of pipelines under internal pressures, than does a surface crack with the same size [1]. The contrast difference in the plasticity constraints drives both different crack driving forces and different fracture resistance along the front of a surface crack from those along the front of an embedded crack. Recent research findings [2], [3], [4] prove that crack-front constraints, characterized often by the linear-elastic T-stress field, vary severely the fracture resistance measured by the fracture resistance J–R curve. However, engineering practices of the integrity assessment of the cracked pipe structures, as outlined in API 579 [5] or BS7910 [6], predicate primarily on the material fracture toughness derived from high-constraint fracture specimens. Acknowledging the effect of crack-front constraints, Zhu and Leis [7] apply the constraint-corrected J–R curve to the fracture assessment of surface cracks in pipelines made of API X80 steels. Similarly, Ruggieri and Cravero [8] implement the constraint-modified failure assessment diagram in the structural integrity assessment of axial surface cracks in pipelines made of X65 steels. Accurate estimations of both the similitude parameter, KI, and the linear-elastic T-stress, therefore, become essential in the failure assessment of cylindrical structures, which embed a welding defect in the wall thickness.
The T-stress represents the second, constant term in the classical Williams’ solution [9] for the elastic crack-tip stress field. It defines a uniform stress parallel to the crack plane. Extensive numerical investigations [10], [11] prove that a zero or positive T-stress field characterizes a crack-front condition that constrains the plastic deformation within a very localized small region ahead of the crack tip, while a negative T-stress causes significant stress redistributions near the crack tip and the plastic deformation thus extends to a relatively larger region ahead of the crack tip than a positive T-stress configuration. Previous researchers [1], [12], [13] recognize the effect of crack-front constraints on the fracture resistance and the growth for a circumferential surface crack and for an embedded circumferential crack in the wall of pipes. The low plasticity constraints in the circumferential surface cracks in the wall of a pipe enhance the fracture resistance and delay the crack growth compared to a highly-constraint crack front under the same crack driving force. Kim [14] proves, from combined experimental and numerical studies, that the high-constraint compact tension, C(T) specimen, provides conservative estimations on the fracture resistance for surface cracks in pipes. Jayadevan et al. [15] and Ostby et al. [16] find, through a series of extensive numerical investigations, that the presence of biaxial loading increases significantly the crack driving force in circumferential surface cracks in the wall of a pipe subjected to tension [15] and bending [16].
The last two decades observe substantial developments in catalogue solutions for the linear-elastic KI and T-stress values via numerical and analytical methods for circumferential cracks in pipes, mainly addressing surface cracks. Wallbrink et al. [17] propose a semi-analytical approach which utilizes the stress field in the undamaged structure to compute the stress-intensity factors for circumferentially cracked pipes. Bergman and Brickstad [18] adopt the line spring elements to compute the SIF values for internal circumferential cracks in pipes. Varfolomeyev and Busch [19] derive the SIF solutions for circumferential through-wall cracks in the cylinder, using the weight function approach. Poette and Albaldejo [20] present the SIF and the influence functions for semi-elliptical, internal surface cracks in pipes under tension and bending loads. Kim and Budden [21] report the approximate solutions to the J-integral and COD values for circumferential through-wall cracks in pipes under tension and bending loads, including the correction for plasticity. For the T-stress investigation, where relatively fewer solutions remain available, a few researchers [22], [23] report the polynomial T-stress approximation for an internal circumferential crack subjected to internal pressure or remote bending.
The current study aims to provide simple approximate solutions to the linear-elastic KI and T-stresses at critical locations along the embedded crack front in the wall of a steel pipe subjected to an internal pressure. The numerical procedure utilizes the interaction-integral approach to compute the elastic KI and T-stress along the front of the circumferentially embedded, elliptical cracks in the wall of a steel cylinder, similar to the study reported in the companion paper [24]. Subsequent data analysis develops a parametric expression for the KI and T-stress values at three locations along the embedded crack front, through a nonlinear curve-fitting procedure.
This paper starts with an introduction on the computational procedures including a very brief summary of the interaction-integral approach and a brief description on the nonlinear curve-fitting procedure, both of which have been described in more details in the companion paper [24]. The following section discusses the numerical T-stress results and the proposed T-stress function for three critical crack-front points for different crack locations, sizes, aspect ratios and pipe wall thicknesses. The subsequent section presents the finite element results for SIF values with respect to different geometric parameters, together with the proposed KI function. The next section compares the SIF and T-stress values computed from the circumferentially embedded cracks and those obtained from the axially embedded cracks reported in the companion paper [24]. The last section summarizes the main conclusions drawn from the current study.
Section snippets
Geometry
This study focuses on the circumferentially embedded crack in the wall of a steel pipe, as schematically shown in Fig. 1, in which Ri refers to the inner radius of the pipe, and t denotes the wall thickness of the pipe. A circumferentially oriented crack denotes a crack, of which the surface lies perpendicular to the longitudinal axis of the pipe, as illustrated in Fig. 1b. The circumferential crack in the wall of the pipe follows a curved shape which deviates from a mathematically perfect
Verification of KI and T-stress computation
The verification study compares the reported T-stress solutions by Huh [29] and the KI values by Chapuliot [30] for surface cracks in the wall of a cylinder with the FE results computed from the numerical procedure described in a previous section. Huh [29] presents a set of polynomial T-stress functions for semi-elliptical surface cracks opening at the inner surface of the pipe, with the coefficients of the polynomials being quadratic functions of the crack length. Huh [29] proposes an
T-stress
This section first summarizes the T-stress values computed from the finite element models described above for cracks with different depths and aspect ratios located at various locations in the wall thickness of the pipe. The T-stress results obtained for the wide range of geometric parameters facilitate the development of a parametric equation, through a nonlinear curve-fitting procedure, to estimate the T-stress values at critical crack-front locations for the circumferentially embedded flaws.
Mode I SIF
This section presents the FE results for mode I SIF values for the circumferentially embedded cracks with variations in the crack depth ratios, the crack aspect ratios, the crack locations and the pipe wall thickness. A nonlinear curve-fitting procedure based on the computed KI results develops an approximate function to estimate the KI values at critical locations of the embedded crack front. The proposed KI function combines a power-law expression of ei (ei = eI, eO or eM) with a second-order
Circumferential crack vs. axial crack
For circumferential cracks in the wall of a pipe, the remote longitudinal stress that drives the mode I opening of the crack derives from the internal pressure applied on a very long, thin-walled pipe, , where refers to the inner pressure on the pipe. In contrast, the remote hoop stress driving the opening of an axially embedded crack in the wall of a pipe, equals , which is twice the remote stress that drives the opening of the circumferentially embedded crack. The
Summary and conclusions
This paper reports a numerical investigation on the linear-elastic T-stress and mode I SIF values for the circumferentially embedded cracks in the wall of a pipe, as an extension to the study on the axially embedded cracks reported in the companion paper. The numerical procedure utilizes the interaction-integral approach to compute the linear-elastic KI and T-stress solutions. The parametric study covers seven crack locations, eM/t, for each of the three crack depth ratios, a/t, and each of the
Acknowledgements
The financial support provided by the Academic Research Fund (Tier 1, Grant No. R264-000-223-133) at the National University of Singapore is gratefully acknowledged.
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