2019
DOI: 10.1111/ffe.13013
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Nonlinear fatigue crack propagation in a baffle module of Wendelstein 7‐X under cyclic bending loads

Abstract: Simulation of the fatigue crack propagation in a Wendelstein 7‐X baffle module is performed in this study using both a finite element method‐based software and the UniGrow nonlinear model for small‐scale yielding (SSY) conditions. Some experimental fatigue tests of several cracked baffle modules have been performed through a servo‐hydraulic machine. One of these experimental tests has been considered to simulate fatigue crack propagation in the baffle module. Before starting the experimental test, a first crac… Show more

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Cited by 3 publications
(4 citation statements)
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“…Furthermore, all the simulations have been carried out in constant amplitude loading condition to calculate the maximum Stress Intensity Factor (SIF) and then ΔK, using an R ‐ratio equal to 0.1. The main advantage of the non‐linear approaches is related to their intrinsic ability to consider the energy dissipated within a small area surrounding the crack front by means of the Low Cycle Fatigue (LCF) properties . Hence, the material chosen for the composite matrix is modelled with either a linear or a non‐linear behaviour according to the Ramberg‐Osgood Equation , ε=σE+0.002σσ01n, where n = 0.178 is the strain hardening coefficient, E = 74 000 MPa is the Young modulus, σ 0 = 314 MPa is the tensile yielding strength of the material, while the ultimate strength is σ ult = 487 MPa .…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…Furthermore, all the simulations have been carried out in constant amplitude loading condition to calculate the maximum Stress Intensity Factor (SIF) and then ΔK, using an R ‐ratio equal to 0.1. The main advantage of the non‐linear approaches is related to their intrinsic ability to consider the energy dissipated within a small area surrounding the crack front by means of the Low Cycle Fatigue (LCF) properties . Hence, the material chosen for the composite matrix is modelled with either a linear or a non‐linear behaviour according to the Ramberg‐Osgood Equation , ε=σE+0.002σσ01n, where n = 0.178 is the strain hardening coefficient, E = 74 000 MPa is the Young modulus, σ 0 = 314 MPa is the tensile yielding strength of the material, while the ultimate strength is σ ult = 487 MPa .…”
Section: Methodsmentioning
confidence: 99%
“…The main advantage of the non-linear approaches is related to their intrinsic ability to consider the energy dissipated within a small area surrounding the crack front by means of the Low Cycle Fatigue (LCF) properties. 11 Hence, the material chosen for the composite matrix is modelled with either a linear or a non-linear behaviour according to the Ramberg-Osgood Equation (1),…”
Section: Methodsmentioning
confidence: 99%
“…Kuna (1998) early presented three-dimensional finite element techniques to calculate the singular coupled electrostatic and anisotropic elastic fields at the crack front tips and confirm the fracture controlling parameters like stress intensity factors and energy release rates. Recently, the fatigue crack behavior was investigated by FEM-based numerical simulations and experimental fatigue tests under different cyclic loading Lepore et al, 2019aLepore et al, , 2019b.…”
Section: Introductionmentioning
confidence: 99%
“…Crack initiation under compressive loading has been explained by tensile residual stresses at the weld. Compressive residual stresses have been shown to slow down crack propagation in Tateishi et al 12 Recently, crack propagation under the influence of residual stresses has been studied in numerical and experimental investigations on brazed pipe specimens 13 and friction stir welded specimens 14 …”
Section: Introductionmentioning
confidence: 99%