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 ...
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