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Page 543
To a first approximation these forces cancel , and so the external stress required
to move a dislocation will be quite small . If the dislocation line is not straight , the
cancellation will be even more λ C 1 . so F D68.833 E ' AO B I I Fig . 19.7 .
To a first approximation these forces cancel , and so the external stress required
to move a dislocation will be quite small . If the dislocation line is not straight , the
cancellation will be even more λ C 1 . so F D68.833 E ' AO B I I Fig . 19.7 .
Page 545
The resulting strain pattern is that of the dislocation characterized jointly by the
boundary curve and the Burgers vector . It is clear that the Burgers vector must be
one of a discrete set of lattice vectors that will allow the rewelding process to ...
The resulting strain pattern is that of the dislocation characterized jointly by the
boundary curve and the Burgers vector . It is clear that the Burgers vector must be
one of a discrete set of lattice vectors that will allow the rewelding process to ...
Page 559
A dislocation segment pinned at each end is called a Frank - Read source , and
we have seen how it can lead to the generation ... This type of dislocation
multiplication gives rise to slip and to the increased density of dislocations during
plastic ...
A dislocation segment pinned at each end is called a Frank - Read source , and
we have seen how it can lead to the generation ... This type of dislocation
multiplication gives rise to slip and to the increased density of dislocations during
plastic ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone
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Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials, ISSN 0084-0203 Wiley series on the science and technology of materials. J. H. Hollomon, advisory editor |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1956 |
| Original from | the University of California |
| Digitized | 21 Sep 2007 |
| ISBN | 0852264674, 9780852264676 |
| Length | 617 pages |
| Export Citation | BiBTeX EndNote RefMan |