Classical ElectrodynamicsProblems after each chapter |
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Page 205
... Linear and Circular Polarization The plane wave ( 7.9 ) is a wave with its electric field vector always in the direction . Such a wave is said to be linearly polarized with polarization vector 1. To describe a general state of ...
... Linear and Circular Polarization The plane wave ( 7.9 ) is a wave with its electric field vector always in the direction . Such a wave is said to be linearly polarized with polarization vector 1. To describe a general state of ...
Page 277
... Linear Antenna For certain radiating systems the geometry of current flow is sufficiently 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 ...
... Linear Antenna For certain radiating systems the geometry of current flow is sufficiently 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 ...
Page 355
... linear . This seems very plausible and is equivalent to the assumption that space - time is homogeneous and isotropic . If the trans- formation is linear , the only possible connection between the quadratic forms ( 11.11 ) and ( 11.12 ) ...
... linear . This seems very plausible and is equivalent to the assumption that space - time is homogeneous and isotropic . If the trans- formation is linear , the only possible connection between the quadratic forms ( 11.11 ) and ( 11.12 ) ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ