Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 87
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 ...
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 ...
Page 71
energy of an ionic crystal . The distance between a positive ion and the nearest negative ion in sodium chloride is known to be 2.81 X 10-8 cm , so that the attractive part of the potential energy of the two ions by themselves is 1 e ...
energy of an ionic crystal . The distance between a positive ion and the nearest negative ion in sodium chloride is known to be 2.81 X 10-8 cm , so that the attractive part of the potential energy of the two ions by themselves is 1 e ...
Page 74
( + ) pij > where now , if we take the reference ion as a negative charge , the plus sign will be used for positive ions and the minus sign for negative ions . An equivalent definition is a ( + ) ( 3.6 ) RO ті where r ; is the distance ...
( + ) pij > where now , if we take the reference ion as a negative charge , the plus sign will be used for positive ions and the minus sign for negative ions . An equivalent definition is a ( + ) ( 3.6 ) RO ті where r ; is the distance ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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 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