Classical Electrodynamics |
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Page 16
... inside a volume V subject to either Dirichlet or Neumann boundary conditions on the closed bounding surface S. We suppose , to the contrary , that there exist two solutions 1 and 1⁄2 satisfying the same boundary conditions . Let U = Φ2 ...
... inside a volume V subject to either Dirichlet or Neumann boundary conditions on the closed bounding surface S. We suppose , to the contrary , that there exist two solutions 1 and 1⁄2 satisfying the same boundary conditions . Let U = Φ2 ...
Page 236
... inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they move instantly in response to changes in the fields , no matter how rapid , and always produce the correct surface - charge density Σ ...
... inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they move instantly in response to changes in the fields , no matter how rapid , and always produce the correct surface - charge density Σ ...
Page 260
... inside and outside the cylinder in order to satisfy boundary conditions at all points on the surface at all times . In the usual way , inside the dielectric cylinder the transverse Laplacian of the fields must be negative so that the ...
... inside and outside the cylinder in order to satisfy boundary conditions at all points on the surface at all times . In the usual way , inside the dielectric cylinder the transverse Laplacian of the fields must be negative so that the ...
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