Electrodynamics of Continuous Media |
From inside the book
Results 1-3 of 90
Page 55
... body . PROBLEM Derive the formula which replaces ( 11.7 ) when the body is not in a vacuum but in a medium of dielectric permeability e ( e ) . SOLUTION . Using the same transformations as before , we find 1 F - Fo = 8π √e . € • ( D ...
... body . PROBLEM Derive the formula which replaces ( 11.7 ) when the body is not in a vacuum but in a medium of dielectric permeability e ( e ) . SOLUTION . Using the same transformations as before , we find 1 F - Fo = 8π √e . € • ( D ...
Page 72
... body in question ( but , of course , does not enclose any of the charged bodies which are sources of the field ) . The calculation of the total force on a dielectric in an electric field in a vacuum can also be approached in another way ...
... body in question ( but , of course , does not enclose any of the charged bodies which are sources of the field ) . The calculation of the total force on a dielectric in an electric field in a vacuum can also be approached in another way ...
Page 162
... body . The total volume of these regions , and therefore the aniso- tropy energy in them , are proportional to the layer thickness a . Thus in all cases the emergence of the domains at the surface of the body results in an excess energy ...
... body . The total volume of these regions , and therefore the aniso- tropy energy in them , are proportional to the layer thickness a . Thus in all cases the emergence of the domains at the surface of the body results in an excess energy ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
Copyright | |
97 other sections not shown
Other editions - View all
Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy atoms averaging axes axis body boundary condition calculated charge circuit co-ordinates coefficient components conducting conductor constant corresponding cross-section crystal Curie point curl H current density denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy equation div expression external field ferroelectric ferromagnetic field H fluid flux force formula free energy frequency function given gives grad H₂ Hence incident induction integral isotropic Laplace's equation layer linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities refraction relation respect result rotation scalar scattering SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion unit volume values variable velocity wave vector wire z-axis zero