Classical ElectrodynamicsProblems after each chapter |
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Page 241
... assumed constant along the cylinder axis . With a sinusoidal time dependence e - it for the fields inside the cylinder , Maxwell's equations take the form : V x E = i W B V.B = 0 C VxB = - ίμε " Ε V.E = 0 C ( 8.16 ) where it is assumed ...
... assumed constant along the cylinder axis . With a sinusoidal time dependence e - it for the fields inside the cylinder , Maxwell's equations take the form : V x E = i W B V.B = 0 C VxB = - ίμε " Ε V.E = 0 C ( 8.16 ) where it is assumed ...
Page 267
... assuming that the azimuthal variation of the fields is eim . ( b ) For m = ± 1 , determine the mode with the lowest cutoff frequency and discuss the properties of its fields ( cutoff frequency , spatial variation , etc. ) , assuming ...
... assuming that the azimuthal variation of the fields is eim . ( b ) For m = ± 1 , determine the mode with the lowest cutoff frequency and discuss the properties of its fields ( cutoff frequency , spatial variation , etc. ) , assuming ...
Page 297
... assumed to be very small compared to a wavelength of the electro- magnetic fields which are assumed to exist on one side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet ...
... assumed to be very small compared to a wavelength of the electro- magnetic fields which are assumed to exist on one side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ