Classical Electrodynamics |
From inside the book
Results 1-3 of 74
Page 15
... zero field and zero potential outside the volume V. ] Two remarks are in order about result ( 1.36 ) . First , if the surface S goes to infinity and the electric field on S falls off faster than R1 , then the surface integral vanishes ...
... zero field and zero potential outside the volume V. ] Two remarks are in order about result ( 1.36 ) . First , if the surface S goes to infinity and the electric field on S falls off faster than R1 , then the surface integral vanishes ...
Page 52
... zero potential , and the other conductor is at a potential such that far from the boss the electric field between the plates is Eo . ( a ) Calculate the surface - charge densities at an arbitrary point on the plane and on the boss , and ...
... zero potential , and the other conductor is at a potential such that far from the boss the electric field between the plates is Eo . ( a ) Calculate the surface - charge densities at an arbitrary point on the plane and on the boss , and ...
Page 236
... zero electric field inside the perfect conductor . Similarly , for time - varying magnetic fields , the surface charges move in response to the tangential magnetic field to produce always the correct surface current K : 4πT nx H = K с ...
... zero electric field inside the perfect conductor . Similarly , for time - varying magnetic fields , the surface charges move in response to the tangential magnetic field to produce always the correct surface current K : 4πT nx H = K с ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ