Introduction to Solid State Physics |
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MOLECULAR CRYSTALS Inert gas atoms and saturated molecules are bound
together in the solid phase by weak electrostatic forces known as van der Waals
forces . These forces arise in the following way : even in an atom or molecule ...
MOLECULAR CRYSTALS Inert gas atoms and saturated molecules are bound
together in the solid phase by weak electrostatic forces known as van der Waals
forces . These forces arise in the following way : even in an atom or molecule ...
Page 304
atom on one lattice lie on the other lattice . If there are N atoms A and N atoms B
in the alloy , the long range order parameter S is defined so that the number of A '
s on lattice a is equal to * ( 1 + ) N . When S = + 1 , the order is perfect and each ...
atom on one lattice lie on the other lattice . If there are N atoms A and N atoms B
in the alloy , the long range order parameter S is defined so that the number of A '
s on lattice a is equal to * ( 1 + ) N . When S = + 1 , the order is perfect and each ...
Page 300
The alloy is disordered if the A and B atoms are randomly arranged , as in Fig .
15 . 1b . Many of ... degree of order . A common ordered arrangement is one in
which all the nearest neighbor atoms of a B atom are A atoms , and vice versa ;
this ...
The alloy is disordered if the A and B atoms are randomly arranged , as in Fig .
15 . 1b . Many of ... degree of order . A common ordered arrangement is one in
which all the nearest neighbor atoms of a B atom are A atoms , and vice versa ;
this ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
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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 |