Classical ElectrodynamicsProblems after each chapter |
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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 P , satisfying the same boundary conditions . Let U ...
... 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 P , satisfying the same boundary conditions . Let U ...
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 259
... inside the hollow . Other guiding structures are possible . The parallel - wire transmission line is an example ... inside the cylinder and one for outside : INSIDE √ , 2 + ( μse @ 2 c2 - k2 = 0 ( 8.98 ) * Note that this factor varies ...
... inside the hollow . Other guiding structures are possible . The parallel - wire transmission line is an example ... inside the cylinder and one for outside : INSIDE √ , 2 + ( μse @ 2 c2 - k2 = 0 ( 8.98 ) * Note that this factor varies ...
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