Authors: Yoshitaka Wada, Takuji Hayashi, Masanori Kikuchi, Fei Xu
Abstract: Due to more complex and severe design restrictions, more effective and faster finite
element analyses are demanded. There are several ways to compute FE analysis efficiently: parallel
computing, fast iterative or direct solvers, adaptive analysis and so on. One of the most effective
analysis ways is the combination of adaptive analysis and multigrid iterative solver, because an
adaptive analysis requires several meshes with difference resolutions and multigrid solver utilizes
such meshes to accelerate its computation. However, convergence of multigrid solver is largely
affected by initial shape of each element. An effective mesh improvement method is proposed here. It
is the combination of mesh coarsening and refinement. A good mesh can be obtained by the method to
be applied to an initial mesh, and better convergence is achieved by the improved initial mesh.
833
Authors: Akiyuki Takahashi, Mitsuru Kawanabe, Masanori Kikuchi
Abstract: Recent 3-Dimensional Atom Probe (3DAP) experimental observations showed the
formation of spherical γ-precipitates at a central region of γ’ phases in nickel based superalloys. The γ
precipitates should give a significant effect to the material strength. Whereat, in this work, we first
developed a simulation technique for the investigation of the formation of γ-precipitates in γ’ phases,
which is based on a combination of an Embedded Atom Method (EAM) interatomic potential
designed for Molecular Dynamics (MD) and the kinetic lattice Monte Carlo (KLMC) method. As a
demonstration of the KLMC simulation, the formation of the L12 structure was simulated from an
initial state with randomly distributed aluminum atoms (25at.%Al). Finally, the γ’ phase with the L12
structure is formed in the entire simulation volume. To understand the fundamental mechanism of the
formation of the L12 structures, the binding energies between a pair of aluminum atoms in a nickel
single crystal were calculated using MD method. The result gave a clear picture of the mechanism.
The stability of the γ-precipitate was also investigated using the MD method. Finally, the formation of
γ-precipitates was simulated using the KLMC method. The dependence of the formation on the
temperature condition is discussed.
815
Authors: Mamtimin Gheni, Dong Cheng Yin, Xu Fei Wang, Masanori Kikuchi
Abstract: In this paper, the mathematical model for nonlinear multi-shaped randomly distributed
domains in revealable and non-revealbale fields is established by using waveform mesh generation
(WMG) method with damp, and made the application function of finite element pre and post
handling system. The results show, this method can conduct mesh transformation to any given
nonlinear function or given shapes in different scale randomly distributed domain in revealable and
non-revealable fields, and obtained some smoothly mesh with matching each boundary and
neighboring domains interaction.
737
Authors: Maigefeireti Maitireyimu, Masanori Kikuchi, Mamtimin Gheni
Abstract: This article presents a modified FEM Superpostion method (S-FEM) for composite
material analysis. Around the reinforcement body, failure and interface fracture may occur in the
matrix. So the S-FEM was employed to detect the stress distribution around the reinforcement. One
particle in big matrix is studied. Area of twice of particle radium is selected as local field.First, the
feasibility of modified S-FEM is verified. And by symmetric analysis, geometric distribution of
particle which may influence on the strength of composite material were discussed.
731
Authors: Akiyuki Takahashi, Yutaka Kobayashi, Masanori Kikuchi
Abstract: This paper describes phase field simulations of the rafting behavior of γ’ phase with a
simple interfacial dislocation network model. The interfacial dislocation network model accounts for
the effect of the network on the lattice misfit between γ and γ’ phases and the subsequent rafting
behavior. The model is implemented into the phase field simulation to see the dependence of the
rafting behavior of γ’ phases on the interfacial dislocation network. Without the dislocation network
model, the amount of the rafting was negligibly small. On the other hand, with the dislocation
network model, the γ’ phases shows a large amount of rafting, which is in good agreement with the
results of the experimental observations. Therefore, the combination of the phase field method and
the simple interfacial dislocation network model developed in this work is appropriate for the
simulation of the rafting of γ’ phases.
471
Authors: Ze Jian Xu, Yu Long Li, Masanori Kikuchi
Abstract: The Mode I and Mode II dynamic fracture toughness (DFT) values, KId and KIId for high
strength steels 40Cr and 30CrMnSiNi2A were evaluated using a combined experimental-numerical
method. The tests were performed on three point bend (3PB) and shear specimens with Hopkinson
pressure bar. The time of crack initiation was determined by a strain gauge. With the assistance of
3-D transient finite element analysis, the temporal evolution of the dynamic stress intensity factor
under different loading rates was obtained, and the DFT was determined by the fracture initiation
time. In Mode I tests, a brittle transgranular fracture was found in 40Cr, while evidence for ductile
fracture was observed on the failure surface of 30CrMnSiNi2A. In Mode II tests, both tensile cracks
and adiabatic shear bands were found for the two steels. The effect of ligament size on fracture
toughness was discussed. The correlations of KId and KIId with loading rate were also investigated.
The micromechanisms of loading rate effect on the DFT were discussed for both modes.
351
Authors: Masanori Kikuchi, Yoshitaka Wada, Masafumi Takahashi, Yu Long Li
Abstract: Fatigue crack growth under mixed mode loading conditions is simulated using S-FEM. By
using S-FEM technique, only local mesh should be re-meshed and it becomes easy to simulate crack
growth. By combining with auto-meshing technique, local mesh is re-meshed automatically, and
curved crack path is modeled easily. Plural fatigue crack problem is solved by this technique. For
two parallel crack problem, criteria of crack coalescence are proposed. By simulating this problem by
S-FEM, it is verified these criteria are conservative ones.
133
Authors: Wei Xie, Qi Qing Huang, Masanori Kikuchi
Abstract: In the virtual crack closure method (VCCM), the energy release rate is computed based on
the results of finite element calculation, and the stress intensity factor (SIF) is computed from the
energy release rate. In this paper, the stress intensity factor of mixed-mode surface cracks under three
point bending is studied by using the three dimensional modified virtual crack closure method
(MVCCM). The modified virtual crack closure method is required to open one element face area
whose shape is arbitrary and finite element widths are unequal across the crack front. The effect of the
distance between the location of load and crack face, crack shape and crack depth to the stress
intensity factor is also discussed, along with practical results and conclusions.
85
Authors: Masanori Kikuchi, Shougo Sannoumaru
Abstract: Dimple fracture tests are conducted under mode I and mixed mode lading conditions.
Dimple fracture zone and shear-lip fracture zone are observed by scanning electron microscope
precisely. It is found that crack growth direction is affected largely by the change of loading
condition. It is also found that the differences of fracture pattern between mid-plane and at free
surface are very large. Void diameter and crack growth direction are measured. Numerical
simulation is conducted to simulate fracture tests in three-dimensional field. Gurson’s constitutive
equation is used and large deformation analyses are conducted. It is assumed that void nucleation is
controlled by both plastic strain and stress. Numerical results are compared with those of
experiments. It is found that results of numerical simulation agree well with those of experiment
qualitatively.
23
Authors: Masanori Kikuchi
Abstract: Thickness effect is studied experimentally. At free surface of the specimen, shear lip
fracture pattern appears, though dimple fracture pattern is observed inside of the specimen. The area
of shear-lip fracture changes due to the change of the specimen thickness. In this study, experimental
study is conducted by changing specimen thicknesses. Fracture surfaces are precisely observed using
SEM, and dimple patterns on them are observed. At the free surface, very narrow no-void area is
observed. It is also found that many voids are nucleated in shear-lip fracture area. FEM simulation is
carried out using Gurson’s constitutive equation. It is found that shear-lip type fracture is simulated
near free surface area by this method. The results show similar tendency with the experimental
observation.
839