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2024 | OriginalPaper | Buchkapitel

17. Line Defects

verfasst von : Rick Ubic

Erschienen in: Crystallography and Crystal Chemistry

Verlag: Springer International Publishing

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Abstract

As we have already seen, some of the most useful properties of crystalline materials arise from defects in their structure. This chapter introduces the concept of line defects, including dislocations and disclinations. A brief biographical sketch of Vito Volterra is included.

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Fußnoten
1
Frank reportedly changed his mind about the word when a professor of English told him that he would be “disinclined” to use it.
 
2
Volterra’s material was a hypothetical continuous matter in which there were no atoms and hence no crystals.
 
3
J.J. Thomson had been his PhD advisor at Cambridge, 1908–1910.
 
4
Something like Fig. 17.3 is universally used in textbooks to illustrate edge dislocations, but it is important to note that this figure is a simplification and in reality virtually no dislocations actually look like this (because virtually nothing has the simple cubic structure – see Sect. 9.​1). A perfect (or full) dislocation in either BCC or FCC metals actually consists of multiple half planes, as we will see in Sect. 17.7.
 
5
For this reason, it was not even technically a vector.
 
6
Actually, there doesn’t even seem to be general agreement about whether these should be called FS/RH and SF/RH or RH/FS and RH/SF.
 
7
You can also prove this fact to yourself by examining Fig. 17.3b.
 
8
In a right-handed screw, clockwise rotations cause an inward (screwing in) motion while anticlockwise rotations cause an outward (screwing out or unscrewing) motion.
 
9
These directions are [100], [010], and [110]. Recall that [110] is crystallographically equivalent to both [100] and [010] in hexagonal crystals and so is of the <100> form despite having different indices.
 
Literatur
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14.
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15.
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16.
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22.
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Metadaten
Titel
Line Defects
verfasst von
Rick Ubic
Copyright-Jahr
2024
DOI
https://doi.org/10.1007/978-3-031-49752-0_17

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