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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 407
... linear in the charge of the particle , ( 2 ) linear in the electromagnetic potentials , ( 3 ) translationally invariant , and ( 4 ) a function of no higher than the first time derivative of the particle coordinates . The reader may ...
... linear in the charge of the particle , ( 2 ) linear in the electromagnetic potentials , ( 3 ) translationally invariant , and ( 4 ) a function of no higher than the first time derivative of the particle coordinates . The reader may ...
Page 562
... 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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ