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 : VxE = i - B V.B = 0 V C ω ▽ × B = −iμe – E 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 : VxE = i - B V.B = 0 V C ω ▽ × B = −iμe – E V.E = 0 C ( 8.16 ) where it is assumed ...
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 ...
Page 443
... assumption that is not valid in dense substances . We have assumed that it is legitimate to calculate the effect of the incident particle's fields on one electron in one atom at a time , and then sum up incoherently the energy transfers ...
... assumption that is not valid in dense substances . We have assumed that it is legitimate to calculate the effect of the incident particle's fields on one electron in one atom at a time , and then sum up incoherently the energy transfers ...
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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