Electrodynamics of Continuous Media |
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Page 123
... linear current does not depend on the assumption that μ = 1. Since we neglect the thickness of the conductor , no boundary conditions at its surface need be applied , and the magnetic properties of the conducting material are of no ...
... linear current does not depend on the assumption that μ = 1. Since we neglect the thickness of the conductor , no boundary conditions at its surface need be applied , and the magnetic properties of the conducting material are of no ...
Page 136
... linear conductors In calculating the self - inductance of a linear conductor its thickness cannot be entirely neglected as it was in calculating the mutual inductance of two conductors . If it were , we should obtain from ( 32.9 ) the ...
... linear conductors In calculating the self - inductance of a linear conductor its thickness cannot be entirely neglected as it was in calculating the mutual inductance of two conductors . If it were , we should obtain from ( 32.9 ) the ...
Page 360
... linear circuits WE MAY apply the general theory of fluctuations † to the interesting problem of current fluctuations in linear electric circuits , first considered by H. NYQUIST ( 1928 ) . The current fluctuations are free electrical ...
... linear circuits WE MAY apply the general theory of fluctuations † to the interesting problem of current fluctuations in linear electric circuits , first considered by H. NYQUIST ( 1928 ) . The current fluctuations are free electrical ...
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 |
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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