Abstract
Different proofs of contracted length non covariance are discussed. The way based on the establishment of interval inconstancy (dependence on velocity) seems to be the most convincing one. It is stressed that the known non covariance of the electromagnetic field energy and momentum of a moving charge (`the problem 4/3`) is a direct consequence of contracted length non covariance. 8 refs.
Citation Formats
Strel`tsov, V N.
Proofs of Contracted Length Non-covariance.
JINR: N. p.,
1994.
Web.
Strel`tsov, V N.
Proofs of Contracted Length Non-covariance.
JINR.
Strel`tsov, V N.
1994.
"Proofs of Contracted Length Non-covariance."
JINR.
@misc{etde_10102799,
title = {Proofs of Contracted Length Non-covariance}
author = {Strel`tsov, V N}
abstractNote = {Different proofs of contracted length non covariance are discussed. The way based on the establishment of interval inconstancy (dependence on velocity) seems to be the most convincing one. It is stressed that the known non covariance of the electromagnetic field energy and momentum of a moving charge (`the problem 4/3`) is a direct consequence of contracted length non covariance. 8 refs.}
place = {JINR}
year = {1994}
month = {Dec}
}
title = {Proofs of Contracted Length Non-covariance}
author = {Strel`tsov, V N}
abstractNote = {Different proofs of contracted length non covariance are discussed. The way based on the establishment of interval inconstancy (dependence on velocity) seems to be the most convincing one. It is stressed that the known non covariance of the electromagnetic field energy and momentum of a moving charge (`the problem 4/3`) is a direct consequence of contracted length non covariance. 8 refs.}
place = {JINR}
year = {1994}
month = {Dec}
}