Introduction to Solid State Physics |
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Page 297
... SINGLE CRYSTALS The classical prediction for the strength of crystals is that the critical shear stress σ should be of the order of magnitude of the shear modulus G , which in a cubic crystal is equal to c44 . If x is the shear displace ...
... SINGLE CRYSTALS The classical prediction for the strength of crystals is that the critical shear stress σ should be of the order of magnitude of the shear modulus G , which in a cubic crystal is equal to c44 . If x is the shear displace ...
Page 323
... SINGLE CRYSTALS The classical prediction for the strength of crystals is that the critical shear stress σ should be of the order of magnitude of the shear modulus G , which in a cubic crystal is equal to c44 . If x is the shear displace ...
... SINGLE CRYSTALS The classical prediction for the strength of crystals is that the critical shear stress σ should be of the order of magnitude of the shear modulus G , which in a cubic crystal is equal to c44 . If x is the shear displace ...
Page 325
... single crystal 1.3 X 107 15,000 Ag , single crystal 2.8 X 1011 6 X 106 45,000 Al , single crystal 2.5 X 1011 4 X 106 60,000 Al , pure , polycrystal 2.5 X 1011 2.6 X 108 900 Al , commercial drawn ~ 2.5 X 1011 9.9 X 108 250 Duralumin ...
... single crystal 1.3 X 107 15,000 Ag , single crystal 2.8 X 1011 6 X 106 45,000 Al , single crystal 2.5 X 1011 4 X 106 60,000 Al , pure , polycrystal 2.5 X 1011 2.6 X 108 900 Al , commercial drawn ~ 2.5 X 1011 9.9 X 108 250 Duralumin ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali alloy anisotropy antiferromagnetic approximately atoms axes axis Bardeen barium titanate boundary calculated charge coefficient conduction band cube Curie point Debye density diamagnetic dielectric constant diffraction diffusion dipole direction discussed dislocation displacement domains effect elastic electric field energy entropy equation equilibrium experimental F-centers factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction ionic crystals ionized ions lattice constant lattice points London low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed optical orbital parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium potassium chloride potential Proc quantum resonance result room temperature scattering Seitz shear Shockley shown in Fig single crystal sodium chloride solids specimen spin strain stress superconducting surface susceptibility symmetry Table theory thermal tion transition unit volume vacancy valence values vector velocity wave functions x-ray zero