Introduction to Solid State Physicsproblems after each chapter |
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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 Dopo V Y D888870999 * & - * - * - * $ * - tao * * 6 ...
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 Dopo V Y D888870999 * & - * - * - * $ * - tao * * 6 ...
Page 557
in nickel , Brown25 estimates 3 X 1011 dislocations / cm2 for severe plastic
deformation . ... If an edge dislocation is present , lattice vacancies precipitating
along its length will eat away a portion of the extra halfplane of atoms and cause
the ...
in nickel , Brown25 estimates 3 X 1011 dislocations / cm2 for severe plastic
deformation . ... If an edge dislocation is present , lattice vacancies precipitating
along its length will eat away a portion of the extra halfplane of atoms and cause
the ...
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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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