Introduction to Solid State Physics |
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Page 310
DIFFUSION OF LATTICE DEFECTS Interstitial atoms will have a certain rate of
diffusion from one interstitial position to another ; also , an atom in a normal
position may move into a hole , thus effectively changing the position of the hole .
DIFFUSION OF LATTICE DEFECTS Interstitial atoms will have a certain rate of
diffusion from one interstitial position to another ; also , an atom in a normal
position may move into a hole , thus effectively changing the position of the hole .
Page 315
ate activation energies . Calculations by Huntington and Seitz14 for metallic
copper , summarized in Table 16 . 3 , show a marked preference for vacancy
diffusion , process ( c ) in Fig . 16 . 12 . The observed selfdiffusion activation
energy of 2 .
ate activation energies . Calculations by Huntington and Seitz14 for metallic
copper , summarized in Table 16 . 3 , show a marked preference for vacancy
diffusion , process ( c ) in Fig . 16 . 12 . The observed selfdiffusion activation
energy of 2 .
Page 310
DIFFUSION OF LATTICE DEFECTS Interstitial atoms will have a certain rate of
diffusion from one interstitial position to another ; also , an atom in a normal
position may move into a hole , thus effectively changing the position of the hole .
DIFFUSION OF LATTICE DEFECTS Interstitial atoms will have a certain rate of
diffusion from one interstitial position to another ; also , an atom in a normal
position may move into a hole , thus effectively changing the position of the hole .
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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Common terms and phrases
alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero
Bibliographic information
| Title | Introduction to Solid State Physics Wiley series on the science and technology of materials |
| Author | Charles Kittel |
| Edition | 2 |
| Publisher | Wiley, 1953 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 396 pages |
| Export Citation | BiBTeX EndNote RefMan |