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 P , and 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 P , and 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 370
... 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 > 0 , that region is called the future . Similarly the lower half - cone is called the past . The system may ...
... 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 > 0 , that region is called the future . Similarly the lower half - cone is called the past . The system may ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ