Classical electrodynamics |
From inside the book
Results 1-3 of 87
Page 241
For simplicity, the cross-sectional size and shape are assumed constant along
the cylinder axis. With a sinusoidal time dependence e~<wt for the fields inside
the cylinder, Maxwell's equations take the form : Vx B=-,>e- c V•B = V•E = (8.16) ...
For simplicity, the cross-sectional size and shape are assumed constant along
the cylinder axis. With a sinusoidal time dependence e~<wt for the fields inside
the cylinder, Maxwell's equations take the form : Vx B=-,>e- c V•B = V•E = (8.16) ...
Page 297
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
Page 443
This reduction in energy loss, known as the density effect, was first treated
theoretically by Fermi (1940). In our discussion so far we have tacitly made one
assumption that is not valid in dense substances. We have assumed that it is
legitimate ...
This reduction in energy loss, known as the density effect, was first treated
theoretically by Fermi (1940). In our discussion so far we have tacitly made one
assumption that is not valid in dense substances. We have assumed that it is
legitimate ...
What people are saying - Write a review
LibraryThing Review
User Review - barriboy - LibraryThingA soul crushing technical manual written by a sadist that has served as the right of passage for physics PhDs since the dawn of time. Every single one of my professors studied this book, and every ... Read full review
LibraryThing Review
User Review - aproustian - LibraryThing"Jackson E&M is about learning how to approximate reliably...the entire book, with few exceptions, is a mathematical discussion on how to solve [the same] 4 problems for different boundary conditions." Read full review
Contents
Introduction to Electrostatics | 1 |
Scalar potential | 7 |
Greens theorem | 14 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration angular distribution approximation assumed atomic average axis behavior Bessel functions boundary conditions bremsstrahlung calculate Chapter charge density charge q charged particle classical coefficients collisions component conductor Consequently consider coordinates cross section current density cylinder defined delta function dielectric constant diffraction dimensions dipole direction discussed effects electric field electromagnetic fields electron electrostatic emitted energy loss expansion expression factor force equation frequency given Green's function impact parameter incident particle inside integral Laplace's equation limit linear Lorentz invariant Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell's equations meson molecules momentum multipole multipole expansion nonrelativistic obtain orbit oscillations parallel perpendicular photon plane wave plasma point charge polarization power radiated problem quantum quantum-mechanical radiative radius region relativistic result scalar scattering shown in Fig shows solid angle solution spectrum spherical surface theorem transverse vanishes vector potential wave equation wave number wavelength written zero