Teoretičeskaâ i matematičeskaâ fizika, Tome 36 (1978) no. 1, pp. 53-63
Citer cet article
A. N. Gordeyev. Description of the electromagnetic interaction of relativistic particles by means of a universal laboratory time. Teoretičeskaâ i matematičeskaâ fizika, Tome 36 (1978) no. 1, pp. 53-63. http://geodesic.mathdoc.fr/item/TMF_1978_36_1_a4/
@article{TMF_1978_36_1_a4,
author = {A. N. Gordeyev},
title = {Description of the electromagnetic interaction of relativistic particles by means of a~universal laboratory time},
journal = {Teoreti\v{c}eska\^a i matemati\v{c}eska\^a fizika},
pages = {53--63},
year = {1978},
volume = {36},
number = {1},
language = {ru},
url = {http://geodesic.mathdoc.fr/item/TMF_1978_36_1_a4/}
}
TY - JOUR
AU - A. N. Gordeyev
TI - Description of the electromagnetic interaction of relativistic particles by means of a universal laboratory time
JO - Teoretičeskaâ i matematičeskaâ fizika
PY - 1978
SP - 53
EP - 63
VL - 36
IS - 1
UR - http://geodesic.mathdoc.fr/item/TMF_1978_36_1_a4/
LA - ru
ID - TMF_1978_36_1_a4
ER -
%0 Journal Article
%A A. N. Gordeyev
%T Description of the electromagnetic interaction of relativistic particles by means of a universal laboratory time
%J Teoretičeskaâ i matematičeskaâ fizika
%D 1978
%P 53-63
%V 36
%N 1
%U http://geodesic.mathdoc.fr/item/TMF_1978_36_1_a4/
%G ru
%F TMF_1978_36_1_a4
For a system of arbitrarily fast charged particles, equations of motion are obtained in Lagrangian form that do not contain field variables and use a universal laboratory time for all the particles. The example of a two-body system shows that the equations of motion contain terms describing an advanced interaction, although the Lagrange function of the system contains only retarded potentials.
