Introduction to Solid State Physics |
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Page 43
Elastic Constants of Crystals This chapter is concerned with the elastic constants
of single crystals . The elastic constants are of interest because of the insight they
give into the nature of the binding forces in solids , and they are also of ...
Elastic Constants of Crystals This chapter is concerned with the elastic constants
of single crystals . The elastic constants are of interest because of the insight they
give into the nature of the binding forces in solids , and they are also of ...
Page 49
23 ) C12 = - 812 / ( 811 – $ 12 ) ( 811 + 2812 ) ; 044 = 1 / 844 · Values of elastic
data for various cubic crystals are tabulated in Table 3 . 1 . The values refer to
room temperature . A general review 6x1011 Elastic coefficients ( dynes / cm2 )
do ...
23 ) C12 = - 812 / ( 811 – $ 12 ) ( 811 + 2812 ) ; 044 = 1 / 844 · Values of elastic
data for various cubic crystals are tabulated in Table 3 . 1 . The values refer to
room temperature . A general review 6x1011 Elastic coefficients ( dynes / cm2 )
do ...
Page 388
... 97 Elastic anisotropy factor , 52 Electrons , in applied field , 256 velocities in
metals , 240 alpha - brass , 58 Electrostatic energy , 355 beta - brass , 58 Elastic
compliance constants , 47 , 50 Elements , crystal structures of , 26 Elastic
constants ...
... 97 Elastic anisotropy factor , 52 Electrons , in applied field , 256 velocities in
metals , 240 alpha - brass , 58 Electrostatic energy , 355 beta - brass , 58 Elastic
compliance constants , 47 , 50 Elements , crystal structures of , 26 Elastic
constants ...
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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