Introduction to Solid State Physicsproblems after each chapter |
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Page 65
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
IONIC CRYSTALS In ionic crystals electrons are transferred from atoms of one
type to atoms of a second type , so that the crystal is made up of positive and
negative ions . The ions arrange themselves so the Coulomb attraction between
ions ...
Page 68
There is apparently a continuous range of crystals between the ionic and the
covalent limits . It is often of importance to estimate the extent to which a given
bond is ionic or covalent , but this may be difficult to do with any confidence . We
think ...
There is apparently a continuous range of crystals between the ionic and the
covalent limits . It is often of importance to estimate the extent to which a given
bond is ionic or covalent , but this may be difficult to do with any confidence . We
think ...
Page 70
It is believed that the hydrogen bonds is largely ionic in character , being formed
only between the most electronegative atoms . The hydrogen atom loses its
electron to one of the other atoms in the molecule ; the proton forms the hydrogen
...
It is believed that the hydrogen bonds is largely ionic in character , being formed
only between the most electronegative atoms . The hydrogen atom loses its
electron to one of the other atoms in the molecule ; the proton forms the hydrogen
...
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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 mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present 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