Classical ElectrodynamicsProblems after each chapter |
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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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... Linear , Center - fed Antenna As an illustration of the use of a multipole expansion for a source whose dimensions are comparable to a wavelength , we consider the radiation from a thin , linear , center - fed antenna , as shown in Fig ...
... Linear , Center - fed Antenna As an illustration of the use of a multipole expansion for a source whose dimensions are comparable to a wavelength , we consider the radiation from a thin , linear , center - fed antenna , as shown in Fig ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ