Abstract
PurposeCrack tip stresses are used to relate the ability of structures to perform under the influence of cracks and defects. One of the methods to determine three-dimensional crack tip stresses is through theJ-Tzmethod. TheJ-Tzmethod has been used extensively to characterize the stresses of cracked geometries that demonstrate positiveT-stress but limited in characterizing negativeT-stresses. The purpose of this paper is to apply theJ-Tzmethod to characterize a three-dimensional crack tip stress field in a changing crack length from positive to negativeT-stress geometries.Design/methodology/approachElastic-plastic crack border fields of deep and shallow cracks in tension and bending loads were investigated through a series of three-dimensional finite element (FE) and analyticalJ-Tzsolutions for a range of crack lengths ranging from 0.1⩽a/W⩽0.5 for two thickness extremes ofB/(W−a)=1 and 0.05.FindingsBoth the FE and theJ-Tzapproaches showed that the combined in-plane and the out-of-plane constraint loss were differently affected by theT-stress and the out-of-plane size effects when the crack length changed from deep to shallow cracks. The conditions of theJ-Tzdominance on the three-dimensional crack front tip were shown to be limited to positiveT-stress geometries, and theJ-Tz-Q2Dapproach can extend the crack border dominance of the three-dimensional deep and shallow bend models along the crack front tip until perturbed by an elastic-plastic corner field.Practical implicationsThe paper reports the limitation of theJ-Tzapproach, which is used to calculate the state of three-dimensional crack tip stresses in power law hardening materials. The results from this paper suggest that the characterization of the three-dimensional crack tip stress in power law hardening materials is still an open issue and requires other suitable solutions to solve the problem.Originality/valueThis paper demonstrates a thorough analysis of a three-dimensional elastic-plastic crack tip fields for geometries that are initially either fully constrained (positiveT-stress) or unconstrained (negativeT-stress) crack tip fields but, subsequently, theT-stress sign changes due to crack length reduction and specimen thickness increase. TheJ-Tzstress-based method has been tested and its dominance over the crack tip field is shown to be affected by the combined in-plane and the out-of-plane constraints and the corner field effects.
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