Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 76
Page 24
... equal to q1 , while the second has 92. Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
... equal to q1 , while the second has 92. Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
Page 25
... equal and opposite charges Q and -Q placed on the conductors and the potential difference between them . ( b ) Sketch the energy density of the electrostatic field in each case as a function of the appropriate linear coordinate . 1.8 ...
... equal and opposite charges Q and -Q placed on the conductors and the potential difference between them . ( b ) Sketch the energy density of the electrostatic field in each case as a function of the appropriate linear coordinate . 1.8 ...
Page 299
... equal and opposite to the incident fields . In the illuminated region , the scattered tangential electric field and normal magnetic induction must be equal and opposite to the corresponding incident fields in order to satisfy the ...
... equal and opposite to the incident fields . In the illuminated region , the scattered tangential electric field and normal magnetic induction must be equal and opposite to the corresponding incident fields in order to satisfy the ...
Other editions - View all
Common terms and phrases
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