Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. |
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Page 222
... electrons . If v is the acceleration of the conductor and m the mass of the electron , then the force on an electron is mv . It affects the electron in the same way as an electric field mv / e , where e is the charge on the electron ...
... electrons . If v is the acceleration of the conductor and m the mass of the electron , then the force on an electron is mv . It affects the electron in the same way as an electric field mv / e , where e is the charge on the electron ...
Page 398
... electron , its energy is E1 = ħ2q , 2 / 2m . Thus we can write 1 F ( E1 ) = ( 2πNe1 / mv2 ) log ( 2mv2 E1 / ħ2 @ 2 ) ... electron , even the maximum transferable momentum ħqmax is small compared with the momentum Mu of the particle . The ...
... electron , its energy is E1 = ħ2q , 2 / 2m . Thus we can write 1 F ( E1 ) = ( 2πNe1 / mv2 ) log ( 2mv2 E1 / ħ2 @ 2 ) ... electron , even the maximum transferable momentum ħqmax is small compared with the momentum Mu of the particle . The ...
Page 449
... electron density in the crystal averaged with allowance for the thermal motion of the atoms . We shall assume the atoms to be so heavy that the majority of their electrons are localized in non - overlapping shells which are only ...
... electron density in the crystal averaged with allowance for the thermal motion of the atoms . We shall assume the atoms to be so heavy that the majority of their electrons are localized in non - overlapping shells which are only ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ electric field electromagnetic electrons ellipsoid equation expression external field ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ