Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 45
Page 16
... derivative of the potential ) every- where on the surface ( corresponding to a given surface - charge density ) also defines a unique problem . Specification of the normal derivative is known as the Neumann boundary condition . We now ...
... derivative of the potential ) every- where on the surface ( corresponding to a given surface - charge density ) also defines a unique problem . Specification of the normal derivative is known as the Neumann boundary condition . We now ...
Page 172
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
Page 188
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
Other editions - View all
Common terms and phrases
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