Electrodynamics of Continuous Media |
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Page 40
... e → ∞o . For , since the boundary condition on the induction D is finite , D must remain finite in the body even for € → ∞ . This means that E → 0 , in accordance with the properties of conductors . PROBLEMS PROBLEM 1. Determine ...
... e → ∞o . For , since the boundary condition on the induction D is finite , D must remain finite in the body even for € → ∞ . This means that E → 0 , in accordance with the properties of conductors . PROBLEMS PROBLEM 1. Determine ...
Page 62
... e is replaced by ev ( e ( ) ( ) ( z ) ) . Hence = e x2 + 22 1,2 + + √ ( e ( x ) E ( Y ) e ( 2 ) ) [ e ( x ) E ( V ) € ( 2 ) • In tensor notation , independent of the system of co - ordinates chosen , we have $ = e / √ ( \ e \ e ...
... e is replaced by ev ( e ( ) ( ) ( z ) ) . Hence = e x2 + 22 1,2 + + √ ( e ( x ) E ( Y ) e ( 2 ) ) [ e ( x ) E ( V ) € ( 2 ) • In tensor notation , independent of the system of co - ordinates chosen , we have $ = e / √ ( \ e \ e ...
Page 268
... e - iwot for that at x = O the field ( E or H ) of the incident wave is E = 0 for t < 0 , E ~ t > 0. Expanding this field as a Fourier integral with respect to time , we reduce the prob- lem to that of waves of various frequencies and ...
... e - iwot for that at x = O the field ( E or H ) of the incident wave is E = 0 for t < 0 , E ~ t > 0. Expanding this field as a Fourier integral with respect to time , we reduce the prob- lem to that of waves of various frequencies and ...
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 | |
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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 cylinder denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy 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 self-inductance SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion uniform unit volume values variable velocity wave vector wire z-axis zero