Introduction to Solid State Physicsproblems after each chapter |
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Page 105
5 ) Fn = B ( Un + 1 – Un ) – B ( Un – Un - 1 ) , the first term in parentheses on the
right being the increase in length of the bond between atoms n and n + 1 , the
second term being the increase in length of the bond between atoms n and n – 1
.
5 ) Fn = B ( Un + 1 – Un ) – B ( Un – Un - 1 ) , the first term in parentheses on the
right being the increase in length of the bond between atoms n and n + 1 , the
second term being the increase in length of the bond between atoms n and n – 1
.
Page 480
We note that the production of Schottky defects lowers the density of the crystal
because the net result of their production is an increase in the volume of the -
Frenkel Schottky Fig . 17 . 2 . Schottky and Frenkel defects in an ionic crystal .
We note that the production of Schottky defects lowers the density of the crystal
because the net result of their production is an increase in the volume of the -
Frenkel Schottky Fig . 17 . 2 . Schottky and Frenkel defects in an ionic crystal .
Page 557
A problem is posed by the presence of dislocations in cast and annealed crystals
. No dislocations can be present in thermal equilibrium , because their energy is
much too great in comparison with the increase in entropy that they produce .
A problem is posed by the presence of dislocations in cast and annealed crystals
. No dislocations can be present in thermal equilibrium , because their energy is
much too great in comparison with the increase in entropy that they produce .
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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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Common terms and phrases
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
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials, ISSN 0084-0203 |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1956 |
| Original from | the University of Michigan |
| Digitized | 20 Nov 2007 |
| Length | 617 pages |
| Export Citation | BiBTeX EndNote RefMan |