Introduction to Solid State Physicsproblems after each chapter |
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Page 89
ELASTIC COMPLIANCE AND STIFFNESS CONSTANTS Hooke ' s law states that
for small deformations the strain is proportional to the stress , so that the strain
components are linear functions of the stress components : ezz = 811X . + 812Y ...
ELASTIC COMPLIANCE AND STIFFNESS CONSTANTS Hooke ' s law states that
for small deformations the strain is proportional to the stress , so that the strain
components are linear functions of the stress components : ezz = 811X . + 812Y ...
Page 92
of elastic constant data and of relationships among various coefficients for the
crystal classes has been given by Hearmon . In Fig . 4 . 3 the experimental values
of the elastic constants of sodium chloride are plotted over a wide temperature ...
of elastic constant data and of relationships among various coefficients for the
crystal classes has been given by Hearmon . In Fig . 4 . 3 the experimental values
of the elastic constants of sodium chloride are plotted over a wide temperature ...
Page 102
Find expressions for Young ' s modulus and Poisson ' s ratio in terms of the
elastic compliances or stiffnesses . 4 . 5 . Show that the velocity of propagation of
a shear wave moving along a ( 110 ) direction with particle motion along a [ 170 ]
...
Find expressions for Young ' s modulus and Poisson ' s ratio in terms of the
elastic compliances or stiffnesses . 4 . 5 . Show that the velocity of propagation of
a shear wave moving along a ( 110 ) direction with particle motion along a [ 170 ]
...
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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 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