Introduction to Solid State Physics |
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Page 35
747558 which has been worked out for the sodium chloride structure by the
Ewald method . The Ewald method is derived and discussed in Appendix B .
Values of Madelung constants for many different crystal structures are tabulated
by ...
747558 which has been worked out for the sodium chloride structure by the
Ewald method . The Ewald method is derived and discussed in Appendix B .
Values of Madelung constants for many different crystal structures are tabulated
by ...
Page 36
are known with the sodium chloride structure than with the cesium chloride
structure , but as the differences in binding energy are small we can often only
decide at a given temperature which will be stable for a particular salt by a
consideration ...
are known with the sodium chloride structure than with the cesium chloride
structure , but as the differences in binding energy are small we can often only
decide at a given temperature which will be stable for a particular salt by a
consideration ...
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 |
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