Reverse bend experiments on the base plate and discussion of the appropriate amount of reverse bending for precrack straightness (Effect of the reverse bend process on the CTOD toughness evaluation and understanding of its mechanisms)
{"title":"Reverse bend experiments on the base plate and discussion of the appropriate amount of reverse bending for precrack straightness (Effect of the reverse bend process on the CTOD toughness evaluation and understanding of its mechanisms)","authors":"Tomoya Kawabata , Hoichi Kitano , Takumi Ozawa , Yoshiki Mikami","doi":"10.1016/j.tafmec.2025.104869","DOIUrl":null,"url":null,"abstract":"<div><div>Measurements of the critical value of the crack-tip opening displacement (CTOD) of welded joints often suffer from weld residual stresses, which prevent the introduction of a straight precrack front. In this study, the effects of reverse bending, a proven method for straightening the crack front shape, on evaluations of the critical CTOD are investigated. To compare the differences in the evaluation results, the authors used a base plate without residual stress inside the material for their experiments. Five different reverse bending treatments were applied to a 50 mm thick base metal, and the effects of reverse bending were evaluated via CTOD tests at low temperatures. Additionally, numerical simulations were carried out via the finite element method to exclude the effects of <em>a</em><sub>0</sub>/<em>W</em> and <em>a</em><sub>f</sub>, which cannot be unified in the experiments, and to understand the mechanism. After reverse bending and unloading, the tensile residual stress is distributed at the notch edge, and a high stress intensity at the fatigue crack tip during CTOD testing can be expected. In addition, when the amount of reverse bending is increased to <em>L</em><sub>r</sub> = 1.35, the compressive residual stress distribution in front of the specimen expands, and the <em>P–V</em><sub>g</sub> curve clearly decreases, which may impair the precrack shape flatness. Therefore, the controlled range of <em>L</em><sub>r</sub> should be at least less than 1.35.</div></div>","PeriodicalId":22879,"journal":{"name":"Theoretical and Applied Fracture Mechanics","volume":"137 ","pages":"Article 104869"},"PeriodicalIF":5.0000,"publicationDate":"2025-02-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Theoretical and Applied Fracture Mechanics","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0167844225000278","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MECHANICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Measurements of the critical value of the crack-tip opening displacement (CTOD) of welded joints often suffer from weld residual stresses, which prevent the introduction of a straight precrack front. In this study, the effects of reverse bending, a proven method for straightening the crack front shape, on evaluations of the critical CTOD are investigated. To compare the differences in the evaluation results, the authors used a base plate without residual stress inside the material for their experiments. Five different reverse bending treatments were applied to a 50 mm thick base metal, and the effects of reverse bending were evaluated via CTOD tests at low temperatures. Additionally, numerical simulations were carried out via the finite element method to exclude the effects of a0/W and af, which cannot be unified in the experiments, and to understand the mechanism. After reverse bending and unloading, the tensile residual stress is distributed at the notch edge, and a high stress intensity at the fatigue crack tip during CTOD testing can be expected. In addition, when the amount of reverse bending is increased to Lr = 1.35, the compressive residual stress distribution in front of the specimen expands, and the P–Vg curve clearly decreases, which may impair the precrack shape flatness. Therefore, the controlled range of Lr should be at least less than 1.35.
期刊介绍:
Theoretical and Applied Fracture Mechanics'' aims & scopes have been re-designed to cover both the theoretical, applied, and numerical aspects associated with those cracking related phenomena taking place, at a micro-, meso-, and macroscopic level, in materials/components/structures of any kind.
The journal aims to cover the cracking/mechanical behaviour of materials/components/structures in those situations involving both time-independent and time-dependent system of external forces/moments (such as, for instance, quasi-static, impulsive, impact, blasting, creep, contact, and fatigue loading). Since, under the above circumstances, the mechanical behaviour of cracked materials/components/structures is also affected by the environmental conditions, the journal would consider also those theoretical/experimental research works investigating the effect of external variables such as, for instance, the effect of corrosive environments as well as of high/low-temperature.