Introduction to Solid State Physicsproblems after each chapter |
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Page 125
On the Einstein model each atom is treated as an independent oscillator which
executes harmonic motion about a fixed point ... the motions of adjacent atoms
are hardly independent , but large regions of the crystal move together coherently
.
On the Einstein model each atom is treated as an independent oscillator which
executes harmonic motion about a fixed point ... the motions of adjacent atoms
are hardly independent , but large regions of the crystal move together coherently
.
Page 299
We now consider in detail the motion of a hole in an applied electric field . We
treat the one - dimensional example illustrated by Fig . 11 . 15 . Initially the band
is filled except for the single vacant state F at the top of the band . An electric field
...
We now consider in detail the motion of a hole in an applied electric field . We
treat the one - dimensional example illustrated by Fig . 11 . 15 . Initially the band
is filled except for the single vacant state F at the top of the band . An electric field
...
Page 553
Motion of the boundary took place by cooperative motion of the dislocations in
the array , each dislocation moving an equal ... The motion was produced by
stresses of the order of magnitude of the yield stress for zinc crystals , a fact that
gives ...
Motion of the boundary took place by cooperative motion of the dislocations in
the array , each dislocation moving an equal ... The motion was produced by
stresses of the order of magnitude of the yield stress for zinc crystals , a fact that
gives ...
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Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion neighbor normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone