Classical Electrodynamics |
From inside the book
Results 1-3 of 64
Page
Since the Lagrangian must be a function of velocities and coordinates, we write
the free-particle equation of motion as d (ymv) = 0 (12.67) dt where y = [1 — (to/co
)]-'4. At the least sophisticated level we know that the Lagrangian L. must be ...
Since the Lagrangian must be a function of velocities and coordinates, we write
the free-particle equation of motion as d (ymv) = 0 (12.67) dt where y = [1 — (to/co
)]-'4. At the least sophisticated level we know that the Lagrangian L. must be ...
Page
Why? Make quantitative statements if you can. As in Problem 14.2a a charge e
moves in simple harmonic motion along the z axis, z(t') = a cos (opot'). (a) Show
that the instantaneous power radiated per unit solid angle is: dP(t) e°cB' sin” 0
cos” ...
Why? Make quantitative statements if you can. As in Problem 14.2a a charge e
moves in simple harmonic motion along the z axis, z(t') = a cos (opot'). (a) Show
that the instantaneous power radiated per unit solid angle is: dP(t) e°cB' sin” 0
cos” ...
Page
Antennas and radiation from multipole sources are examples of the first type of
problem, while motion of charges in electric and magnetic fields and energy-loss
phenomena are examples of the second type. Occasionally, as in the discussion
...
Antennas and radiation from multipole sources are examples of the first type of
problem, while motion of charges in electric and magnetic fields and energy-loss
phenomena are examples of the second type. Occasionally, as in the discussion
...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Introduction to Electrostatics | 1 |
Nº 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
Other editions - View all
Common terms and phrases
acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |