Authors: Hui Fang, Kenta Matsumoto, Takashi Sumigawa, Takayuki Kitamura
Abstract: Chiral sculptured thin films (STFs) Glancing-angle deposition (GLAD) thin films are nanoengineered to meet the requirements of a variety of applications such as micro filters, sensors, and waveguides due to their unique frequency characteristics which cannot be achieved by conventional solid materials. For the design, it is necessary to understand the elastic properties of STFs. To facilitate this, we report on our newly developed advanced micro-scale vibration testing process. In the testing, specially designed micro-specimens with surface areas of tens by tens of microns are excited using a piezoelectric (PZT) actuator and the resonance frequencies are detected by a laser device in the vertical or lateral directions successfully. The anisotropy elastic modulus of STFs composed of helical nanosprings are identified on the basis of vibration testing. The thin film shows strong characteristic anisotropy that the solid one hardly can attain. The micro-scale testing technique can be extended to other materials and microstructures.
9
Authors: Takashi Sumigawa, Kenta Matsumoto, Takayuki Kitamura
Abstract: In order to investigate the effect of microscopic structure on fatigue behavior of nanoscale components, a resonant fatigue experiment is conducted using a nanocomponents specimen where the test section is composed of a single crystalline Si substrate, a 200 nm thickness Cu polycrystalline film and a SiN amorphous layer. In the specimen, only the Cu portion plastically deforms because the yield stress is lower than those of other materials. The shape and the crystalline orientation of each grain on the surface of Cu portion are specified by means of EBSD. Although crystallographic slip bands with a width of a few tens of nanometers appear only in a grain of Cu portion, the grain is different from that expected by the Schmid factor. A FEM analysis, which takes into account the deformation anisotropy of grains, reveals that shear stress to generate slip bands is concentrated on the grain owing to the deformation constraint by neighboring crystals and components.
1705
Authors: Masato Yamamoto, Takayuki Kitamura, Takashi Ogata
Abstract: Directionally solidified (DS) superalloys, which have elongated large grains, are used for
gas-turbine blades. Since the grain size is not small enough in comparison with the crack size
observed often in a real component, the inhomogeneous microstructure due to the aligned grains may
strongly affect the crack propagation property. Center-cracked-plate specimens with three different
orientations, TP0 with the parallel DS axis to the load, TP90T with the perpendicular DS axis to the
load and the crack propagation direction, and TP90L with the perpendicular DS axis to the load and
parallel to the crack propagation direction, are subjected to high-temperature (1143K) fatigue. The
specimens after the tests show the transgranular cracking perpendicular to the load axis in TP0,
intergranular one parallel to the DS axis in TP90L, and intergranular / transgranular one parallel to the
DS axis in TP90T. The crack propagation rate da/dN shows a good correlation with effective stress
intensity factor range Keff in each cases. However, the magnitude of da/dN at a same Keff in TP90L
is relatively higher than that in TP0, and that in TP90T remarkably fluctuates. A microscopic
observation of TP90T reveals that the high da/dN is caused by the intergranular cracking, while the
low da/dN is observed on the transgranular cracking. A procedure for the prediction of crack
propagation is proposed on the basis of the two types of cracking; transgranular and intergranular
cracks perpendicular to the load axis. The validity of the proposed procedure is discussed by the
comparison of tested and predicted results of crack propagation in a fatigue condition.
205
Authors: Yoshimasa Takahashi, Hiroyuki Hirakata, Takayuki Kitamura
Abstract: The plasticity of a copper (Cu) nano-component is experimentally evaluated by a cantilever
specimen with multi-layered structure. The cantilever is monotonically loaded by a diamond tip and
the deflection at the free-end is precisely measured by a transmission electron microscope (TEM).
The plastic deformation of the Cu nano-component is successfully monitored through the non-linear
behavior of applied load, P, and cantilever deflection, δ. The plastic constitutive quation of the Cu
component is inversely analyzed by finite element method (FEM) assuming that the component obeys
the Ramberg-Osgood law. The parameters in the R-O law (σ0, n and α) are optimally fitted to
reproduce the experimentally evaluated P-δ relation. The resultant parameter set is derived as (σ0, n,
α) = (345 MPa, 3.2, 1.25). The Cu nano-component has a much higher yield stress and a hardening
rate compared with the ones in a bulk Cu.
297
Authors: Fu Lin Shang, Takayuki Kitamura
Abstract: Atomistic simulations using molecular dynamics (MD) method are conducted to check the
conditions of the onset of fracture at the interface edges with a variety of angles. The simulations are
facilitated with model bi-material systems interacting with Morse pair potentials. Three simulation
models are considered, i.e. the interface edges with angles 45°, 90° and 135°, respectively. The
simulation results show that, at the instant of crack initiation, the maximum stresses along the
interfaces reach the ideal strength of the interface; also, the interface energies just decrease to below
the value of the intrinsic cohesive energy of the interface. And the onset of fracture at the interface
edges with different geometries is controlled by the maximum stresses or the cohesive interfacial
energy.
969
Authors: Takayuki Kitamura, Hiroyuki Hirakata, Yoshimasa Takahashi
Abstract: The interface strength of low-dimensional nano-components such as films and islands
formed on substrates has been investigated in this project, and the focus is put on the mechanics of
crack initiation from the free interface edge and propagation along the interface. The series of
experiments elucidates the applicability of fracture mechanics concept on the structures. We proposed
experimental methods for evaluating the initiation strength of an interface crack in submicron films
and islands deposited on substrates. The initiation is governed by the singular stress field, and the
criterion is prescribed by the stress intensity parameter. Using special loading apparatus built in a
TEM, we developed a crack initiation method for nano-components and the role of plasticity on the
delamination is clarified. Subcritical crack growth along an interface between submicron films under
fatigue was also investigated by modified four-point bend method.
1
Authors: Seong Min Jeong, Takayuki Kitamura
Abstract: The diamond structure of single crystal silicon transforms to other structures under
mechanical stress. We investigate the structural transformation of diamond cubic structure to betatin
structure in silicon under uniaxial stress using atomistic simulation on the basis of the Tersoff
potential. As a result, under extensive compressive strain, the structural transformation from Si-I to
Si-II is found.
963
Authors: Yusuke Kinoshita, Yoshitaka Umeno, Takayuki Kitamura
Abstract: Using the first-principles calculation, the elastic constant C44 of Ag/Al multilayers with
different modulation periods from 0.43 nm to 2.27 nm has been evaluated in order to examine the
effect of atomic and electronic structures on it. With increasing modulation period, C44 decreases
and becomes close to that obtained by the conventional mixing rule, however, the difference of 8 %
still remains at the modulation period of 2.27 nm. As C44 correlates with the average interplanar
spacing, the decrease of C44 can be explained by the decrease of the charge density in the stacking
direction due to the increase of the average interplanar spacing. The difference in the electronic
structure is included in the effect of atomic structure.
959
Authors: Takayuki Kitamura, Akihiro Kushima, Yoshitaka Umeno
Abstract: The ideal strength of a nano-component, which is the maximum stress of the structure,
provides an insight into the mechanical behavior of minute material. We conducted tensile
simulations for cylindrical-shaped Cu nano-wires composed of an atomic chain as a core wrapped
around by shell(s) with the structure of (111) layers in an fcc crystal. The results are compared with
Cu atomic chain and sheet which are components of the nanowire. Young’s moduli and the ideal
strengths of the wires are less than a single atomic chain and a sheet. The mechanical strength of the
wire is weakened by the following three factors: (A) Change in electron arrangement caused by
combining core and shell; (B) Larger interatomic distance (inherent tensile strain) of the outer shell
introduced by the mismatch of atomic layers due to the curvature difference; (C) Mismatch between
shells due to curvature difference. Factor (A) reduces the bonding strength in the shell(s) that
occupy a greater part of the wire. 5-1 wire, which consists of a core and a shell, is weaker than the
single atomic chain and the single sheet due to (A) and (B). 10-5-1 wire, consisting of a core and
two shells, has less strength than 5-1 wire due to (C) in addition to (A) and (B).
919
Authors: Fu Lin Shang, Takayuki Kitamura
Abstract: Molecular dynamics (MD) simulations are performed to study the onset of fracture at the
free edges of bi-material interfaces. The objective is to see whether a unified criterion could be
formulated for crack initiation at interface edges with different angles or not. The simulations are
facilitated with model bi-material systems interacting with Morse pair potentials. Three simulation
models are considered, i.e. the interface edges with angles 45°, 90° and 135°, respectively. The
simulation results show that, at the instant of crack initiation, the maximum stresses along the
interfaces reach the ideal strength of the interface; also, the interface energies just decrease to below
the value of the intrinsic cohesive energy of the interface. These findings revealed that the onset of
fracture at the interface edges with different geometries could be controlled by the maximum stresses
or the cohesive interfacial energy.
949