Classical Electrodynamics |
From inside the book
Results 1-3 of 81
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 : ω Vx EiB V.B = 0 ▽ x B = - = − iμe == E - ίμε V.E = 0 C ( 8.16 ) where it is ...
... 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 : ω Vx EiB V.B = 0 ▽ x B = - = − iμe == E - ίμε V.E = 0 C ( 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 ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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