Classical Electrodynamics |
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Page 91
From (3.170) and an identity of Problem 3.12c this requirement can be seen to
imply lim f(k) = q (3.172) k->0 When boundary conditions (3.171) are applied to
the general solution (3.170), there results a pair of integral equations of the first ...
From (3.170) and an identity of Problem 3.12c this requirement can be seen to
imply lim f(k) = q (3.172) k->0 When boundary conditions (3.171) are applied to
the general solution (3.170), there results a pair of integral equations of the first ...
Page 284
To do this we make use of the following easily proved identities connecting
surface integrals over a closed surface S to volume ... (GE)] doz (9.74) y From the
expansion, V × V x A = V(V. A.) – W*A, it is evident that the volume integral
vanishes ...
To do this we make use of the following easily proved identities connecting
surface integrals over a closed surface S to volume ... (GE)] doz (9.74) y From the
expansion, V × V x A = V(V. A.) – W*A, it is evident that the volume integral
vanishes ...
Page 301
We see that Fon and Fm are proportional to (k+ kg), respectively; the shadow
integral will be large and the integral from the illuminated region will go to zero.
As the scattering angle departs from the forward direction the shadow integral will
...
We see that Fon and Fm are proportional to (k+ kg), respectively; the shadow
integral will be large and the integral from the illuminated region will go to zero.
As the scattering angle departs from the forward direction the shadow integral will
...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
6 other sections not shown
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Common terms and phrases
acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence 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 light 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 relativistic result satisfy scalar scattering shown in Fig shows side 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 |