Introduction to Solid State Physics |
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Page 49
22 ) U = } cu ( ezza + eye ? + ezz ? ) + C12 ( egyezz ... For cubic crystals the
compliance and stiffness constants are related by C11 = ( 811 + $ 12 ) / ( 811 –
312 ) ( 811 + 2812 ) ; ( 3 . 23 ) C12 = - 812 ... of sodium chloride . [ After L . Hunter
and ...
22 ) U = } cu ( ezza + eye ? + ezz ? ) + C12 ( egyezz ... For cubic crystals the
compliance and stiffness constants are related by C11 = ( 811 + $ 12 ) / ( 811 –
312 ) ( 811 + 2812 ) ; ( 3 . 23 ) C12 = - 812 ... of sodium chloride . [ After L . Hunter
and ...
Page 52
The anisotropy factor A in a cubic crystal is defined as ( 3 . ... 2 ; Cu 3 . 3 ; Pb 3 . 9
. CAUCHY RELATIONS There are among the elastic stiffness constants certain
relations first obtained by ... C . Schaefer and L . Bergmann , Abhandl . preuss .
The anisotropy factor A in a cubic crystal is defined as ( 3 . ... 2 ; Cu 3 . 3 ; Pb 3 . 9
. CAUCHY RELATIONS There are among the elastic stiffness constants certain
relations first obtained by ... C . Schaefer and L . Bergmann , Abhandl . preuss .
Page 246
49 Cu 2 . 23 2 . 33 W 3 . 04 3 . 20 Ir 2 . 49 2 . 49 Zn 2 . 31 2 . 33 Mo 2 . 61 2 . 79 Pt
18 Experimental studies of the temperature dependence of L at low temperatures
in sodium and copper have been carried out by R . Berman and D . K . C ...
49 Cu 2 . 23 2 . 33 W 3 . 04 3 . 20 Ir 2 . 49 2 . 49 Zn 2 . 31 2 . 33 Mo 2 . 61 2 . 79 Pt
18 Experimental studies of the temperature dependence of L at low temperatures
in sodium and copper have been carried out by R . Berman and D . K . C ...
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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