Nano-Structural Observation of in situ Silica in Natural Rubber Matrix by Three Dimensional Transmission Electron Microscopy

2004 ◽  
Vol 25 (12) ◽  
pp. 1186-1190 ◽  
Author(s):  
Yuko Ikeda ◽  
Atsushi Katoh ◽  
Junichi Shimanuki ◽  
Shinzo Kohjiya
2013 ◽  
Vol 19 (S5) ◽  
pp. 43-48 ◽  
Author(s):  
Maria Rudneva ◽  
Bo Gao ◽  
Ferry Prins ◽  
Qiang Xu ◽  
Herre S.J. van der Zant ◽  
...  

AbstractIn situ transmission electron microscopy was performed on the electromigration in platinum (Pt) nanowires (14 nm thick, 200 nm wide, and 300 nm long) with and without feedback control. Using the feedback control mode, symmetric electrodes are obtained and the gap usually forms at the center of the Pt nanowire. Without feedback control, asymmetric electrodes are formed, and the gap can occur at any position along the wire. The three-dimensional gap geometries of the electrodes in the Pt nanowire were determined using high-angle annular dark-field scanning transmission electron microscopy; the thickness of the nanowire is reduced from 14 nm to only a few atoms at the edge with a gap of about 5–10 nm.


2007 ◽  
Vol 80 (4) ◽  
pp. 690-700 ◽  
Author(s):  
Atsushi Kato ◽  
Shinzo Kohjiya ◽  
Yuko Ikeda

Abstract Usual rubber products are a composite from rubber and nano-filler (e.g. silica, carbon black, etc.), and it is believed that the good dispersion of the nano-filler is the most important issue determining the performance of rubber vulcanizates. So far, transmission electron microscopy (TEM) has been the most useful tool for evaluation of the dispersion. However, it affords images of the sample projected on an x, y-plane, and the information along the thickness (z-axis) direction is missing. Three-dimensional (3D) visualization of nanometer structure of nano-filler dispersion in a rubber matrix is what all rubber technologists have been dreaming of. This dream is at last realized, and described in this paper. Use of TEM combined with computerized tomography (abbreviated as 3D-TEM in this paper, which is sometimes called electron tomography) enabled us to reconstruct 3D images of nano-filler (silica or carbon black) aggregates in rubbery matrix. It is said that nano-filler aggregate is a structure of size from 10 nm to 1000 nm, and agglomerate is an even larger structure. The 3D-TEM results on silica aggregates in natural rubber were presented in this paper. Silica aggregates were characterized by combining the 3D images of the vulcanizates. Furthermore, density of silica loaded natural rubber as an example of physical properties, was measured, and explained by the structure elucidated by 3D-TEM.


2005 ◽  
Vol 20 (7) ◽  
pp. 1910-1917 ◽  
Author(s):  
L. Sun ◽  
J.C. Yang

The nucleation and growth of Cu2O islands due to Cu(100) oxidation at temperatures from 200 to 350 °C have been observed by in situ ultra-high-vacuum transmission electron microscopy. For this temperature range, epitaxial Cu2O islands form a triangular shape with rounded edges when Cu(100) is exposed to dry oxygen at 5 × 10−4 Torr in situ. Our initial analysis on the nucleation and growth of these three-dimensional Cu2O islands agrees well with the heteroepitaxial model of surface diffusion of oxygen.


2016 ◽  
Vol 52 (16) ◽  
pp. 3300-3303 ◽  
Author(s):  
Langli Luo ◽  
Lianfeng Zou ◽  
Daniel K. Schreiber ◽  
Matthew J. Olszta ◽  
Donald R. Baer ◽  
...  

We report the in situ atomic-scale visualization of the dynamic three-dimensional growth of NiO during the initial oxidation of Ni–10at%Cr using environmental transmission electron microscopy.


2011 ◽  
Vol 172-174 ◽  
pp. 242-247 ◽  
Author(s):  
Egle Conforto ◽  
Daniel Caillard

The motion of steps during the growth of hydride precipitates has been observed by in situ transmission electron microscopy. Precipitates in different orientation relationships (OR) are shown to obey to the rules of three-dimensional edge-to-edge matching. They form clusters in order to realize a more isotropic distribution of the volume expansion, and to decrease their total elastic energy.


Author(s):  
W. D. Cooper ◽  
C. S. Hartley ◽  
J. J. Hren

Interpretation of electron microscope images of crystalline lattice defects can be greatly aided by computer simulation of theoretical contrast from continuum models of such defects in thin foils. Several computer programs exist at the present time, but none are sufficiently general to permit their use as an aid in the identification of the range of defect types encountered in electron microscopy. This paper presents progress in the development of a more general computer program for this purpose which eliminates a number of restrictions contained in other programs. In particular, the program permits a variety of foil geometries and defect types to be simulated.The conventional approximation of non-interacting columns is employed for evaluation of the two-beam dynamical scattering equations by a piecewise solution of the Howie-Whelan equations.


Author(s):  
J. T. Sizemore ◽  
D. G. Schlom ◽  
Z. J. Chen ◽  
J. N. Eckstein ◽  
I. Bozovic ◽  
...  

Investigators observe large critical currents for superconducting thin films deposited epitaxially on single crystal substrates. The orientation of these films is often characterized by specifying the unit cell axis that is perpendicular to the substrate. This omits specifying the orientation of the other unit cell axes and grain boundary angles between grains of the thin film. Misorientation between grains of YBa2Cu3O7−δ decreases the critical current, even in those films that are c axis oriented. We presume that these results are similar for bismuth based superconductors and report the epitaxial orientations and textures observed in such films.Thin films of nominally Bi2Sr2CaCu2Ox were deposited on MgO using molecular beam epitaxy (MBE). These films were in situ grown (during growth oxygen was incorporated and the films were not oxygen post-annealed) and shuttering was used to encourage c axis growth. Other papers report the details of the synthesis procedure. The films were characterized using x-ray diffraction (XRD) and transmission electron microscopy (TEM).


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