Introduction to Solid State Physics |
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Page 71
Thermal Properties of Solids We first discuss the exact theory of the heat capacity
of monatomic and diatomic lattices in one dimension and compare the result with
an approximate method of treatment due to Debye . The Debye theory is then ...
Thermal Properties of Solids We first discuss the exact theory of the heat capacity
of monatomic and diatomic lattices in one dimension and compare the result with
an approximate method of treatment due to Debye . The Debye theory is then ...
Page 78
this as an approximation to the entire heat capacity of solids . The internal energy
hw ( 5 . 20 ) chw / kt - 1 leads , on differentiation with respect to temperature , to
the heat capacity ( 5 . 21 ) Co = Nk ( hw / kT ) ? emw / kt / ( etw / kt – 1 ) ; the ...
this as an approximation to the entire heat capacity of solids . The internal energy
hw ( 5 . 20 ) chw / kt - 1 leads , on differentiation with respect to temperature , to
the heat capacity ( 5 . 21 ) Co = Nk ( hw / kT ) ? emw / kt / ( etw / kt – 1 ) ; the ...
Page 88
where Cy is the heat capacity per unit volume at constant pressure , C , at
constant volume , B is the temperature coefficient of linear expansion , and K is
the compressibility . Estimate Co - C , for copper at 300°K and at 1000°K . 5 . 5 .
Derive ...
where Cy is the heat capacity per unit volume at constant pressure , C , at
constant volume , B is the temperature coefficient of linear expansion , and K is
the compressibility . Estimate Co - C , for copper at 300°K and at 1000°K . 5 . 5 .
Derive ...
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Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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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