Introduction to Solid State Physics |
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Page 46
... force , and the subscript indicates the normal to the plane to which the force is applied . Thus the stress component X2 represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the x direction ...
... force , and the subscript indicates the normal to the plane to which the force is applied . Thus the stress component X2 represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the x direction ...
Page 54
... forces on the central force assumption ( ẞ = 0 ) the simple cubic lattice does not possess any l , m + 1 , n + 1 l − 1 , m , n + 1 l , m , n + 1 1+ 1 , m , n + 1 l - 1 , m + 1 , n l , m + 1 , n 1+ 1 , m + 1 , n l , m - 1 , n + 1ợ 1-1 ...
... forces on the central force assumption ( ẞ = 0 ) the simple cubic lattice does not possess any l , m + 1 , n + 1 l − 1 , m , n + 1 l , m , n + 1 1+ 1 , m , n + 1 l - 1 , m + 1 , n l , m + 1 , n 1+ 1 , m + 1 , n l , m - 1 , n + 1ợ 1-1 ...
Page 180
... force H , for a wide range of magnetic materials is shown in Fig . 10.15 . There is a very close correlation ... force , Hc ( oersteds ) ⚫5 % Tungsten steel Remalloy • Vicalloy I Alnico I • Alnico V Ferro - platinum- 102 • Vectolite 103 ...
... force H , for a wide range of magnetic materials is shown in Fig . 10.15 . There is a very close correlation ... force , Hc ( oersteds ) ⚫5 % Tungsten steel Remalloy • Vicalloy I Alnico I • Alnico V Ferro - platinum- 102 • Vectolite 103 ...
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
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absorption alkali halides alkali metal alloy anisotropy antiferromagnetic approximation 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 entropy equation equilibrium experimental F-center factor Fermi ferroelectric ferromagnetic free electron frequency given heat capacity holes impurity interaction interstitial ionic crystals ionized lattice constant lattice points London low temperatures magnetic field magnetic moment molecules motion nearest neighbor normal observed orbital p-n junctions parallel paramagnetic particles perovskite phonons Phys physical plane polarizability polarization positive potassium chloride potential Proc quantum range order region resonance result room temperature scattering Seitz semiconductor Shockley shown in Fig single crystal sodium chloride solids specimen spin superconducting susceptibility symmetry Table theory thermal tion unit volume valence values vector velocity wave functions x-ray zero