Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 89
Page 10
... dipole - layer distribution on a surface S. A dipole layer can be imagined as being formed by letting the surface S have a surface - charge density o ( x ) on it , and another surface S ' , lying close to S , have an equal and opposite ...
... dipole - layer distribution on a surface S. A dipole layer can be imagined as being formed by letting the surface S have a surface - charge density o ( x ) on it , and another surface S ' , lying close to S , have an equal and opposite ...
Page 274
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution pm . Thus we find eikr B = k2 ( n x m ) x n + [ 3n ( n . m ) ...
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution pm . Thus we find eikr B = k2 ( n x m ) x n + [ 3n ( n . m ) ...
Page 628
... Dipole approximation , in energy loss , 435 in radiation problems , 271 , 274 , 507 Dipole fields , electrostatic , 100 magnetostatic , 143 , 147 of conducting sphere , 34 of dielectric sphere , 115 of electrostatic dipole layer , 9 of ...
... Dipole approximation , in energy loss , 435 in radiation problems , 271 , 274 , 507 Dipole fields , electrostatic , 100 magnetostatic , 143 , 147 of conducting sphere , 34 of dielectric sphere , 115 of electrostatic dipole layer , 9 of ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
24 other sections not shown
Other editions - View all
Common terms and phrases
4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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