Introduction to Solid State Physics |
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Page 79
24 ) T = 3kTg / 4c ? , giving a constant value of the temperature coefficient of
thermal expansion . Values of the linear expansion coefficients are given in Table
5 . 3 . TABLE 5 . 3 . LINEAR COEFFICIENTS OF THERMAL EXPANSION NEAR ...
24 ) T = 3kTg / 4c ? , giving a constant value of the temperature coefficient of
thermal expansion . Values of the linear expansion coefficients are given in Table
5 . 3 . TABLE 5 . 3 . LINEAR COEFFICIENTS OF THERMAL EXPANSION NEAR ...
Page 84
In thermal conductivity one needs not only a way of limiting the mean free path ,
but also a way of establishing an equilibrium ... When A becomes comparable
with the width of the test specimen , the value of A is limited by Specific thermal ...
In thermal conductivity one needs not only a way of limiting the mean free path ,
but also a way of establishing an equilibrium ... When A becomes comparable
with the width of the test specimen , the value of A is limited by Specific thermal ...
Page 85
In glasses the thermal conductivity ( Fig . 5 . 5 ) decreases as the temperature is
lowered ; this effect is present even at room temperature . Furthermore , the
values of the thermal conductivity at room temperature run about an order of ...
In glasses the thermal conductivity ( Fig . 5 . 5 ) decreases as the temperature is
lowered ; this effect is present even at room temperature . Furthermore , the
values of the thermal conductivity at room temperature run about an order of ...
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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