Classical ElectrodynamicsProblems after each chapter |
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Page 241
... assumed constant along the cylinder axis . With a sinusoidal time dependence e - iat for the fields inside the cylinder , Maxwell's equations take the form : W VxE = i B V.B = 0 C V x B = iμe - E - — iμe® V.E = 0 с ( 8.16 ) where it is ...
... assumed constant along the cylinder axis . With a sinusoidal time dependence e - iat for the fields inside the cylinder , Maxwell's equations take the form : W VxE = i B V.B = 0 C V x B = iμe - E - — iμe® V.E = 0 с ( 8.16 ) where it is ...
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 ...
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... 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 ...
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