Physical Properties of Crystals |
From inside the book
Results 1-3 of 25
Page 72
... plate condenser If a slab of dielectric is placed between the plates of a parallel plate condenser the capacity of the condenser is increased . It is shown in textbooks on electrostatics that the ratio of the capacities with and without ...
... plate condenser If a slab of dielectric is placed between the plates of a parallel plate condenser the capacity of the condenser is increased . It is shown in textbooks on electrostatics that the ratio of the capacities with and without ...
Page 107
... plate , but the deformations involved when the plate has an arbitrary crystallographic orientation are not simple . In Fig . 6.12 the plate is supposed to be resting on a plane bed , and the point O in the lower surface remains fixed ...
... plate , but the deformations involved when the plate has an arbitrary crystallographic orientation are not simple . In Fig . 6.12 the plate is supposed to be resting on a plane bed , and the point O in the lower surface remains fixed ...
Page 200
... plate arrangement is evidently k11 , the conductivity normal to the plate , while with the long rod it is r11 , the resistivity along the rod . The situation is analogous to that in elasticity , where by applying a known stress one ...
... plate arrangement is evidently k11 , the conductivity normal to the plate , while with the long rod it is r11 , the resistivity along the rod . The situation is analogous to that in elasticity , where by applying a known stress one ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
20 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined deformation denoted diad axis dielectric dijk displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ heat flow Hence hexagonal indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic photoelastic effect piezoelectric effect plane plate polarization positive principal axes pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress suffixes symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal wave surface x₁ Young's Modulus zero ат