We present an algorithm for computing the electromagnetic fields due to currents inside and outside of finite sources with a high degree of spatial symmetry for arbitrary time-dependent currents. The solutions for these fields do not involve the time derivatives of the currents but involve only the currents and their time integrals. We give solutions for moving planar sheets of charge, and a rotating spherical shell carrying a uniform charge density. We show that the general solutions reduce to the standard expressions for magnetic dipole radiation for slow time variations of the currents. If the currents are turned on very quickly, the general solutions show that the amount of energy radiated equals the magnetic energy stored in the static fields a long time after current creation. We give three problems which can be used in undergraduate courses and one problem suitable for graduate courses. These problems illustrate that because the generation of radiation depends on what has happened in the past, a system of currents can radiate even during time intervals when the currents are constant due to radiation associated with earlier acceleration.

1.
J. D.
Jackson
,
Classical Electrodynamics
, 2nd ed. (
John Wiley & Sons
,
Hoboken, NJ
,
1975
), Chap. 16.
2.
H.
Spohn
,
Dynamics of Charged Particles and Their Radiation Field
(
Cambridge U.P.
,
Cambridge
,
2004
) and
W.
Appel
and
M.
Kiessling
, “
Scattering and radiation damping in gyroscopic Lorentz electrodynamics
,”
Lett. Math. Phys.
60
,
31
46
(
2002
) and
W.
Appel
and
M.
Kiessling
, “
Mass and spin renormalization in Lorentz electrodynamics
,”
Ann. Phys. (NY)
289
,
24
83
(
2001
) and
M.
Kunze
, “
On the absence of radiationless motion for a rotating classical charge
,”
Adv. Math.
223
,
1632
1665
(
2010
).
3.
R. P.
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R. B.
Leighton
, and
M.
Sands
,
The Feynman Lectures on Physics
(
Addison-Wesley
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See also
J.-M.
Chung
, “
Revisiting the radiation from a suddenly moving sheet of charge
,”
Am. J. Phys.
76
(
2
),
133
136
(
2008
);
B. R.
Holstein
, “
Radiation from a suddenly moving sheet of charge
,”
Am. J. Phys.
63
(
3
),
217
221
(
1995
);
P. C.
Peters
, “
Electromagnetic radiation from a kicked sheet of charge
,”
Am. J. Phys.
54
(
3
),
239
245
(
1986
), in particular Eq. (6) for the electric field of a single sheet of moving charge and the accompanying discussion in Sec. II;
T. A.
Abbott
and
D. J.
Griffiths
, “
Acceleration without radiation
,”
Am. J. Phys.
53
(
12
),
1203
1211
(
1985
), Sec. III.
4.
An x-component of the electric field would arise from the scalar potential φ and from the relation E=-φ-A/t. We ignore φ and hence omit the x-component of E. Because we treat the charge density as constant in time, the scalar potential and Ex are constant, hence irrelevant to our considerations. Note that we could have chosen to have the surface current consist of opposite charge densities driven into motion in opposite directions, producing the same total current density as in Eq. (2), but without any charge density, and hence without any Ex. These same considerations, with appropriate modifications, justify our omission of the radial electric field for the spinning spherical shell considered in Sec. III.
5.
J.
Daboul
and
J. D.
Jensen
, “
Radiation reaction for a rotating sphere with rigid surface charge
,”
Z. Physik.
265
,
455
478
(
1973
), Eqs. (2.23) and (2.24).
6.
A.
Vlasov
, “
Radiation reaction in classical electrodynamics: The case of a rotating charged sphere
,” e-print arXiv:physics/9801017v1, Eq. (8).
7.
See supplementary material at http://dx.doi.org/10.1119/1.3682326 for the method for solving the spherical case, for the solutions to the problems posed in the text, and for animations of Figs. 2 and 3.
8.
Reference [1], Eq. (9.33), gives the Fourier domain solution for the vector potential. With the replacement ik=iω/c by -(1/c)d/dt, we recover our Eq. (26).
9.
B.
Cabral
and
C.
Leedom
, “
Imaging vector fields using line integral convolution
,” Proceedings of the SIGGRAPH 93,
1993
, pp.
263
270
.

Supplementary Material

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