Introduction to Solid State Physics |
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Page 73
Calculated heat capacity of a one - dimensional monatomic lattice , in the
continuum approximation , and on the exact theory . The curves are adjusted so
that hwmax = k® , with = 200°K , on both calculations . ( After M . Blackman , Proc
. Roy .
Calculated heat capacity of a one - dimensional monatomic lattice , in the
continuum approximation , and on the exact theory . The curves are adjusted so
that hwmax = k® , with = 200°K , on both calculations . ( After M . Blackman , Proc
. Roy .
Page 74
In this approximation dk / dw is simply 1 / vo , and we have ( 5 . 11 ) U - Lm hw
TTVO Jo chwkt – 1 dw . The upper limit to the integral , wm , is here to be
determined by the condition that the number of states considered should come
out equal to ...
In this approximation dk / dw is simply 1 / vo , and we have ( 5 . 11 ) U - Lm hw
TTVO Jo chwkt – 1 dw . The upper limit to the integral , wm , is here to be
determined by the condition that the number of states considered should come
out equal to ...
Page 77
We then treat the N degrees of freedom of the acoustical branch in the Debye
approximation , ( 5 . 11 ) or ( 5 . 16 ) . W 20 Mg 230 & Na 159 63 Cu Ni EINSTEIN
FUNCTION The heat capacity of a system of simple harmonic oscillators of the ...
We then treat the N degrees of freedom of the acoustical branch in the Debye
approximation , ( 5 . 11 ) or ( 5 . 16 ) . W 20 Mg 230 & Na 159 63 Cu Ni EINSTEIN
FUNCTION The heat capacity of a system of simple harmonic oscillators of the ...
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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