Electrodynamics of Continuous Media |
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Page 2
... surface of the body , the mean field E in the vacuum is almost the same as the actual field e . The two fields differ only in the immediate ... surface of a homogeneous conductor is an equipotential surface 2 §1 Electrostatics of Conductors.
... surface of the body , the mean field E in the vacuum is almost the same as the actual field e . The two fields differ only in the immediate ... surface of a homogeneous conductor is an equipotential surface 2 §1 Electrostatics of Conductors.
Page 3
... surface of the electrostatic field . The component of the field normal to the surface is very simply related to the charge density on the surface . The relation is obtained from the general electrostatic equation div e = 4mp , which on ...
... surface of the electrostatic field . The component of the field normal to the surface is very simply related to the charge density on the surface . The relation is obtained from the general electrostatic equation div e = 4mp , which on ...
Page 171
... surface of the ring , = 0 at infinity , and 42-41 = 47J / c on the chosen surface , where $ 1 and 2 are the values of the potential on the two sides of that surface . Such a problem is known from potential theory to have a unique ...
... surface of the ring , = 0 at infinity , and 42-41 = 47J / c on the chosen surface , where $ 1 and 2 are the values of the potential on the two sides of that surface . Such a problem is known from potential theory to have a unique ...
Contents
Notation X | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
Copyright | |
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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 cylinder denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid 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