Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 94
Page 84
Suppose that it were possible to permeate the space between ions in an ionic crystal with a homogeneous fluid of dielectric constant e without affecting the equation for the repulsive interactions between ions , but reducing the Coulomb ...
Suppose that it were possible to permeate the space between ions in an ionic crystal with a homogeneous fluid of dielectric constant e without affecting the equation for the repulsive interactions between ions , but reducing the Coulomb ...
Page 102
Show that in a cubic crystal the effective compliance constant for a shear across the ( 110 ) plane in the [ 1ī0 ) direction is equal to 2 ( 811 – 812 ) and the stiffness constant is š ( cu – C12 ) , while in the [ 001 ] direction in ...
Show that in a cubic crystal the effective compliance constant for a shear across the ( 110 ) plane in the [ 1ī0 ) direction is equal to 2 ( 811 – 812 ) and the stiffness constant is š ( cu – C12 ) , while in the [ 001 ] direction in ...
Page 169
This type of polarization was first discussed by Debye ( 1912 ) , who showed that by assuming that molecules could have permanent dipole moments one could explain the high dielectric constant of water , alcohol , and similar liquids ...
This type of polarization was first discussed by Debye ( 1912 ) , who showed that by assuming that molecules could have permanent dipole moments one could explain the high dielectric constant of water , alcohol , and similar liquids ...
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