Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 50
Page 103
... Macroscopic Electrostatics ; Effects of Aggregates of Atoms The equations V • € = Απρί ▽ x ε = 0 ( 4.20 ) govern electrostatic phenomena of all types , provided the ... Macroscopic Media , Dielectrics 103 Macroscopic electrostatics,
... Macroscopic Electrostatics ; Effects of Aggregates of Atoms The equations V • € = Απρί ▽ x ε = 0 ( 4.20 ) govern electrostatic phenomena of all types , provided the ... Macroscopic Media , Dielectrics 103 Macroscopic electrostatics,
Page 194
... macroscopic displacement current ǝD / ǝt . The basic assumption inherent in our previous discussions was that the macroscopic fields E and B which satisfy the two homogeneous Maxwell's equations ( 6.28 ) are the averages of the ...
... macroscopic displacement current ǝD / ǝt . The basic assumption inherent in our previous discussions was that the macroscopic fields E and B which satisfy the two homogeneous Maxwell's equations ( 6.28 ) are the averages of the ...
Page 196
... macroscopic conduction - current density J ( x , t ) . Solutions ( 6.106 ) and ( 6.110 ) , augmented by the free ... macroscopic polarization P and magnetization M , the averaged charge and current densities in ( 6.111 ) can be expressed ...
... macroscopic conduction - current density J ( x , t ) . Solutions ( 6.106 ) and ( 6.110 ) , augmented by the free ... macroscopic polarization P and magnetization M , the averaged charge and current densities in ( 6.111 ) can be expressed ...
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