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 2 satisfying the same contradiction boundary conditions ...
... 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 2 satisfying the same contradiction boundary conditions ...
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 370
... inside ( outside ) the light cone is said to have a time - like ( space- like ) separation from the origin ... inside the upper half- cone , e.g. , the curve OB . Since the path of the system lies inside the upper half - cone for times t ...
... inside ( outside ) the light cone is said to have a time - like ( space- like ) separation from the origin ... inside the upper half- cone , e.g. , the curve OB . Since the path of the system lies inside the upper half - cone for times t ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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