Classical ElectrodynamicsProblems after each chapter |
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Page 51
... plane conductor held at zero potential . Using the method of images , find : ( a ) the surface - charge density induced on the plane , and plot it ; ( b ) the force between the plane and the charge by using Coulomb's law for the force ...
... plane conductor held at zero potential . Using the method of images , find : ( a ) the surface - charge density induced on the plane , and plot it ; ( b ) the force between the plane and the charge by using Coulomb's law for the force ...
Page 202
John David Jackson. 7 Plane Electromagnetic Waves This chapter is concerned with plane waves in unbounded , or perhaps semi - infinite , media . The basic properties of plane waves in non- conducting media - their transverse nature , the ...
John David Jackson. 7 Plane Electromagnetic Waves This chapter is concerned with plane waves in unbounded , or perhaps semi - infinite , media . The basic properties of plane waves in non- conducting media - their transverse nature , the ...
Page 220
... plane of incidence . This means that if n ' > n there is a phase reversal for the reflected wave . 7.6 Polarization by Reflection and Total Internal Reflection Two aspects of the dynamical relations on reflection and refraction are ...
... plane of incidence . This means that if n ' > n there is a phase reversal for the reflected wave . 7.6 Polarization by Reflection and Total Internal Reflection Two aspects of the dynamical relations on reflection and refraction are ...
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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