Classical electrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. 
From inside the book
Results 13 of 88
Page 48
lQVj (i 1,2,..., ii) (1.61) The coefficients Cu are called capacities or capacitances
while the Ci(, i^j, are called coefficients of induction. The(capacitance of a
conductor is therefore the total charge on the conductor when it is maintained at
unit ...
lQVj (i 1,2,..., ii) (1.61) The coefficients Cu are called capacities or capacitances
while the Ci(, i^j, are called coefficients of induction. The(capacitance of a
conductor is therefore the total charge on the conductor when it is maintained at
unit ...
Page 66
If the number of terms in the series is finite (say N), M**t<i*Uğ(& (2.30) nl then we
can ask for the "best" choice of coefficients a* so that we get the "best"
representation of the function /(£). If "best" is defined as minimizing the mean
square error ...
If the number of terms in the series is finite (say N), M**t<i*Uğ(& (2.30) nl then we
can ask for the "best" choice of coefficients a* so that we get the "best"
representation of the function /(£). If "best" is defined as minimizing the mean
square error ...
Page 91
The coefficients A, and Bi can be determined from the boundary conditions.
Suppose that the potential is specified to be V(0) on the surface of a sphere of
radius a, and it is required to find the potential inside the sphere. If there are no
charges ...
The coefficients A, and Bi can be determined from the boundary conditions.
Suppose that the potential is specified to be V(0) on the surface of a sphere of
radius a, and it is required to find the potential inside the sphere. If there are no
charges ...
What people are saying  Write a review
User ratings
5 stars 
 
4 stars 
 
3 stars 
 
2 stars 
 
1 star 

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 and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
18 other sections not shown
Common terms and phrases
4vector amplitude angle angular distribution angular momentum aperture approximation assumed atomic axis behavior Bessel functions boundary conditions bremsstrahlung calculation Chapter charge density charge q charged particle classical coefficients collision components conductor consider coordinates cross section current density cylinder defined dielectric constant differential diffraction dimensions dipole direction discussed effects electric and magnetic electric field electromagnetic fields electrons electrostatic energy loss expansion expression factor finite force frequency given Green function incident integral Lagrangian limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell equations medium modes molecules multipole multipole expansion multipole moments nonrelativistic normal obtain oscillations parallel parameter photon Phys plane wave plasma point charge polarization problem propagation quantum quantummechanical radius region relativistic resonant rest frame result scalar scalar potential scattering shown in Fig solution spectrum sphere spherical surface tensor theorem transverse unit vanishes vector potential velocity wave guide wave number wavelength written zero