Introduction to Solid State Physicsproblems after each chapter |
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Preface to the Second Edition This volume is intended as an introductory
textbook in solid state physics for students of physics , chemistry , and
engineering . My object has been to write an elementary and short account of
representative ...
Preface to the Second Edition This volume is intended as an introductory
textbook in solid state physics for students of physics , chemistry , and
engineering . My object has been to write an elementary and short account of
representative ...
Page 173
DIPOLE ORIENTATION IN SOLIDS We expect molecules in gases and liquids to
be fairly free to rotate , and the permanent dipole moments may be expected to
make their full orientational contribution to the polarizability , as calculated above
.
DIPOLE ORIENTATION IN SOLIDS We expect molecules in gases and liquids to
be fairly free to rotate , and the permanent dipole moments may be expected to
make their full orientational contribution to the polarizability , as calculated above
.
Page 509
is strong in comparison with the binding between molecules ; the former is
caused by covalent forces and the latter by van der Waals forces . Electronic
excitation lines of an individual molecule will often appear in the crystalline solid
with little ...
is strong in comparison with the binding between molecules ; the former is
caused by covalent forces and the latter by van der Waals forces . Electronic
excitation lines of an individual molecule will often appear in the crystalline solid
with little ...
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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