Electrodynamics of Continuous MediaCovers the theory of electromagnetic fields in matter, and the theory of the 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. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
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Page 251
... shock wave are not only collinear but parallel . In slow shock waves we have , on both sides of the discontinuity , v1 < H2 / 4πj = n v12 / vn Noting also that by the continuity of the mass flux p1n1 = P2n2 , we deduce from p1 < P2 that ...
... shock wave are not only collinear but parallel . In slow shock waves we have , on both sides of the discontinuity , v1 < H2 / 4πj = n v12 / vn Noting also that by the continuity of the mass flux p1n1 = P2n2 , we deduce from p1 < P2 that ...
Page 252
... shock waves respectively . The thick dashed curve is the non - evolutionary range U1 < v1 < √ ( 4 × 12 - 3u012 ) , ending on the right at the point v2 UA2 - t 2 = 1 PROBLEM 2. In front of a shock wave the tangential magnetic field H11 ...
... shock waves respectively . The thick dashed curve is the non - evolutionary range U1 < v1 < √ ( 4 × 12 - 3u012 ) , ending on the right at the point v2 UA2 - t 2 = 1 PROBLEM 2. In front of a shock wave the tangential magnetic field H11 ...
Page 390
... shock wave velocity v2 = c2 ( E2 — E1 ) / ( D2 — D1 ) . - ( 111.7 ) In a shock wave there is dissipation of energy . Let Q be the rate of dissipation per unit area of the discontinuity surface . To calculate Q , we write the law of ...
... shock wave velocity v2 = c2 ( E2 — E1 ) / ( D2 — D1 ) . - ( 111.7 ) In a shock wave there is dissipation of energy . Let Q be the rate of dissipation per unit area of the discontinuity surface . To calculate Q , we write the law of ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
Copyright | |
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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 expression external field factor 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 satisfied 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