Introduction to Solid State PhysicsProblems after each chapter. |
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Page 88
... force , and the subscript indicates the normal to the plane to which the force is applied . Thus the stress component X , represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the direction ; the ...
... force , and the subscript indicates the normal to the plane to which the force is applied . Thus the stress component X , represents a force applied in the x direc- tion to a unit area of a plane whose normal lies in the direction ; the ...
Page 105
... force constant . Looked at on a macroscopic . scale , the line has a linear density p = M / a , as there are 1 / a atoms per unit length , and an elastic stiffness c = Ba . The latter result follows as the force required to stretch a ...
... force constant . Looked at on a macroscopic . scale , the line has a linear density p = M / a , as there are 1 / a atoms per unit length , and an elastic stiffness c = Ba . The latter result follows as the force required to stretch a ...
Page 422
... FORCE AND HYSTERESIS The coercive force is perhaps the most sensitive property of ferro- magnetic materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for ...
... FORCE AND HYSTERESIS The coercive force is perhaps the most sensitive property of ferro- magnetic materials which is subject to our control , and it is one of the most important criteria in the selection of ferromagnetic materials for ...
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
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absorption acceptors alkali alloys approximately atoms axes axis barium titanate boundary Bragg Brillouin zone calculated chapter charge conduction band conduction electrons crystal structure cube cubic Curie point Debye density dielectric constant diffraction diffusion dipole direction discussion dislocation distribution domain effective mass elastic electric field energy equation equilibrium exciton experimental F centers factor Fermi ferroelectric ferromagnetic free electron frequency germanium given heat capacity hexagonal holes impurity interaction ionization ions lattice constant lattice point levels low temperatures magnetic field magnetic moment metals molecules motion nearest neighbor normal observed p-n junction paramagnetic particles phonons Phys physics plane polarizability polarization positive potential Proc region resonance result room temperature rotation semiconductor Shockley shown in Fig sodium chloride solid solution space group specimen spin superconducting surface susceptibility symmetry Table theory tion transition unit volume vacancies valence band values vector velocity wave functions wavelength x-ray zero