A calculation of the radiated power and magnetic field of Čerenkov radiation using the Hamiltonian approach is presented. We use this approach to show explicitly how the Čerenkov cone appears in the limit of long times. The Hamiltonian approach is well suited for studying the formation of the cone at the very beginning of the process using numerical integration. The topic is appropriate for advanced courses on electromagnetic fields and in introductory courses on quantum electrodynamics.

1.
V. L.
Ginzburg
,
Applications of Electrodynamics in Theoretical Physics and Astrophysics
(
Gordon and Breach
,
New York
,
1989
);
W. B.
Case
, “
The field oscillator approach to classical electrodynamics
,”
Am. J. Phys.
68
,
800
811
(
2000
).
2.
A.
Likar
and
N.
Razpet
, “
The electromagnetic dipole radiation field through the Hamiltonian approach
,”
Eur. J. Phys.
30
,
1435
1446
(
2009
).
3.
R. M.
More
, “
Čerenkov radiation
,”
Am. J. Phys.
34
(
3
),
243
245
(
1966
).
4.
H.
Motz
and
L. I.
Schiff
, “
Čerenkov radiation in dispersive medium
,”
Am. J. Phys.
21
(
4
),
258
259
(
1953
).
5.
N. C. R.
Pfeifer
and
T. A.
Nieminen
, “
Visualization of Čerenkov radiation and the fields of a moving charge
,”
Eur. J. Phys.
27
,
521
529
(
2006
).
6.
I. S.
Gradsteyn
and
I. M.
Ryzhik
,
Table of Integrals, Series, and Products
(
Academic
,
San Diego
,
1994
).
7.
W. K. H.
Panofsky
and
M.
Phillips
,
Classical Electricity and Magnetism
(
Addison-Wesley
,
Reading, MA
,
1962
), p.
346
.
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