Introduction to Solid State Physics |
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Page 2
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 that the Coulomb attraction
between ...
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 that the Coulomb attraction
between ...
Page 29
Lattice Energy of Ionic Crystals When we speak of ionic crystals we mean
substances such as lithium fluoride and sodium chloride . These are perhaps as
simple as any chemical compound existing in nature , and for this reason they
have ...
Lattice Energy of Ionic Crystals When we speak of ionic crystals we mean
substances such as lithium fluoride and sodium chloride . These are perhaps as
simple as any chemical compound existing in nature , and for this reason they
have ...
Page 41
12 A . The fact that the actual lattice constant is appreciably smaller than the
estimates may perhaps suggest that the bonding is not purely ionic , but is partly
covalent . For sodium chloride , which is probably principally ionic , we have Do =
0 .
12 A . The fact that the actual lattice constant is appreciably smaller than the
estimates may perhaps suggest that the bonding is not purely ionic , but is partly
covalent . For sodium chloride , which is probably principally ionic , we have Do =
0 .
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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