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Grain boundaries amorphization

We have discussed the packing of ions in terms of coordination polyhedra. When we create defects in a crystal we can create new polyhedra that are not found in the perfect crystal. Pauling s rules were developed for perfect crystals, but the principles still apply when we examine defects. One complication is that as we introduce grain boundaries, for example, new sites are produced that depend on the detailed nature of the grain boundary. Amorphous materials present a new challenge when describing point defects. Two amorphous materials can have different structures that depend on the processing history even if the chemistry is the same. [Pg.83]

Fig. 26. High-resolution phase-contrast image showing grain-boundary amorphization reaction in Y/Cu thin films. The reaction results in a nonatomically smooth reaction front. The 0.3 nm interplanar distance corresponds to the (111) plane of YHj (see text). (By courtesy of Dr. C. Ahn, California Institute of Technology, Pasadena, CA, USA). Fig. 26. High-resolution phase-contrast image showing grain-boundary amorphization reaction in Y/Cu thin films. The reaction results in a nonatomically smooth reaction front. The 0.3 nm interplanar distance corresponds to the (111) plane of YHj (see text). (By courtesy of Dr. C. Ahn, California Institute of Technology, Pasadena, CA, USA).
The following mechanisms in corrosion behavior have been affected by implantation and have been reviewed (119) (/) expansion of the passive range of potential, (2) enhancement of resistance to localized breakdown of passive film, (J) formation of amorphous surface alloy to eliminate grain boundaries and stabilize an amorphous passive film, (4) shift open circuit (corrosion) potential into passive range of potential, (5) reduce/eliminate attack at second-phase particles, and (6) inhibit cathodic kinetics. [Pg.398]

If the weak bonding model is valid for high angle grain boundaries (>20°) it follows that diffusion in amorphous preparations of a given material should also show this measure of enhanced diffusion, when compared widr die crystalline material. [Pg.199]

The Phenomenon. In existing materials the electron density is not even constant inside a single phase. This is obvious for the liquid structure of amorphous regions. Nevertheless, even in crystalline phases lattice distortions and grain boundaries result in variations of the electron density about its mean value. In analogy to the sunlight scattered from the fluctuations of air density, X-rays are scattered from the fluctuations of electron density. [Pg.134]

This grain boundary fraction is truly disordered, if not plainly amorphous. This is illustrated in Fig. 1.15. The fraction of atoms that counts into grain boundaries should increase with milling time however, in powder particulates below some... [Pg.45]

Said this, we can let the reader to recall Fig. 1.15, where we depicted amorphous-like phase regions at grain boundaries as the pathways open for preferential diffusion of hydrogen atoms. Apparently, an alloy can benefit from some fraction of amorphous phase to improve kinetics of hydrogen absorption, but complete amorphization of crystalline lattice lowers capacity for storing hydrogen [156]. Mechanochemical activation is therefore a complex process where kinetic and thermodynamic effects must be firstly well understood, and then optimized. [Pg.52]


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Boundary/boundaries grains

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