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Page 118
... simple cubic lattice . Since the indices run equally over positive and negative values , the cross terms involving ( ijp1⁄2 + ikp ̧ ) vanish . By symmetry the sums : ijk i2 j2 = ( î2 + j2 + k2 ) 31⁄2 = Σ ( @ 2 + ƒ2 + k2 ) 31⁄2 are all ...
... simple cubic lattice . Since the indices run equally over positive and negative values , the cross terms involving ( ijp1⁄2 + ikp ̧ ) vanish . By symmetry the sums : ijk i2 j2 = ( î2 + j2 + k2 ) 31⁄2 = Σ ( @ 2 + ƒ2 + k2 ) 31⁄2 are all ...
Page 268
... simple radiating systems . A more systematic approach to radiation by localized distributions of charge and current is left to Chapter 16 , where multipole fields are discussed . The second half of the chapter is devoted to the subject ...
... simple radiating systems . A more systematic approach to radiation by localized distributions of charge and current is left to Chapter 16 , where multipole fields are discussed . The second half of the chapter is devoted to the subject ...
Page 277
... simple that integral ( 9.3 ) for the vector potential can be found in relatively simple , closed form . As an example of such a system we consider a thin , linear antenna of length d which is excited across a small gap at its mid- point ...
... simple that integral ( 9.3 ) for the vector potential can be found in relatively simple , closed form . As an example of such a system we consider a thin , linear antenna of length d which is excited across a small gap at its mid- point ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ