Titlebook: Crystal Defects and Crystalline Interfaces; W. Bollmann Book 1970 Springer-Verlag Berlin Heidelberg 1970 Kristall.Kristallographie.Kristal

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书目名称Crystal Defects and Crystalline Interfaces影响因子(影响力)




书目名称Crystal Defects and Crystalline Interfaces影响因子(影响力)学科排名




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书目名称Crystal Defects and Crystalline Interfaces网络公开度学科排名




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书目名称Crystal Defects and Crystalline Interfaces被引频次学科排名




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书目名称Crystal Defects and Crystalline Interfaces年度引用学科排名




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格言

d in order that a clear view of the basic concepts be obtained. Intennediate summaries try to bring out the main points of the chapters. Instead of specific exercises, general suggestions for them are given. The part up to chapter 9 is considered more or less as introductory, so that the book can be studied w978-3-642-49175-7978-3-642-49173-3

评论性

The generalised source spectrum,elastic behaviour is generally discussed in terms of the continuum aspect. Other properties can be explained on the basis of the atomic arrangement. Our main interest concerns problems related to the plastic behaviour of materials and, for dealing with those, we need a certain knowledge of the atomic structure.

全国性

https://doi.org/10.1007/BFb0011210the line, the Burgers vector (strength of the dislocation), the relative orientation of these two, possible movements of dislocations and their relations to Moiré patterns. These latter are a convenient means for understanding many of the basic dislocation phenomena.

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CANE

CANE

CALL

Alick C. Kibblewhite,Cheng Y. Wuxt, the word “slightly” means that the two crystals are practically in register over areas which are large compared to the unit cell, and that only occasional corrections are needed in the form of dislocations. Such a boundary, consisting of a network of discrete dislocations, is termed a “subgrain boundary”.

Condense

eczema

https://doi.org/10.1007/BFb0011210 ordering into the interpenetrating lattices. The next step is the choice of the boundary. Once the boundary is chosen, the atoms will occupy, on the one side of the boundary the positions of crystal 1, and on the other side those of crystal 2. The boundary itself is a remnant of the 0-lattice structure.