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 223
... Fourier components ( on the assumption that the Fourier expansion contains chiefly terms whose frequencies satisfy the above condition ) . PROBLEM 2. Determine the total charge which flows along a thin circular ring when it ceases a ...
... Fourier components ( on the assumption that the Fourier expansion contains chiefly terms whose frequencies satisfy the above condition ) . PROBLEM 2. Determine the total charge which flows along a thin circular ring when it ceases a ...
Page 395
... Fourier component of A is ( ΔΦ ) = - k φι · - k2 Φκ · Taking the Fourier component of equation ( 113.1 ) gives = -Saxed ( ΔΦ ) = -4лed ( r - vt ) exp ( -ik r ) dv = -4ле exp ( - itv · k ) . Thus ê ( 4лe / k2 ) exp ( − itv · k ) , and ...
... Fourier component of A is ( ΔΦ ) = - k φι · - k2 Φκ · Taking the Fourier component of equation ( 113.1 ) gives = -Saxed ( ΔΦ ) = -4лed ( r - vt ) exp ( -ik r ) dv = -4ле exp ( - itv · k ) . Thus ê ( 4лe / k2 ) exp ( − itv · k ) , and ...
Page 399
... Fourier space integrals . Taking the Fourier components of equations ( 114.6 ) , we have = Απεν с exp ( − itv ⚫k ) , k2 Ax + ĉa2 Ak c2 at2 ê k2 x + ĉ a2øk c2 at2 = 4ле exp ( - itv k ) . · + This effect was pointed out by E. Fermi ...
... Fourier space integrals . Taking the Fourier components of equations ( 114.6 ) , we have = Απεν с exp ( − itv ⚫k ) , k2 Ax + ĉa2 Ak c2 at2 ê k2 x + ĉ a2øk c2 at2 = 4ле exp ( - itv k ) . · + This effect was pointed out by E. Fermi ...
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