Radiation by relativistic dipoles. II

Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expr...
Ausführliche Beschreibung

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Autor*in:	Bordovitsyn, V. A. [verfasserIn] Gushchina, V. S. Zhukova, I. N.

Format:	Artikel
Sprache:	Englisch

Erschienen:	1993

Schlagwörter:	Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment

Anmerkung:	© Plenum Publishing Corporation 1993

Übergeordnetes Werk:	Enthalten in: Russian physics journal - Kluwer Academic Publishers-Plenum Publishers, 1992, 36(1993), 3 vom: März, Seite 247-252
Übergeordnetes Werk:	volume:36 ; year:1993 ; number:3 ; month:03 ; pages:247-252

Links:	Volltext

DOI / URN:	10.1007/BF00559629

Katalog-ID:	OLC2033040453

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allfields	10.1007/BF00559629 doi (DE-627)OLC2033040453 (DE-He213)BF00559629-p DE-627 ger DE-627 rakwb eng 530 370 VZ Bordovitsyn, V. A. verfasserin aut Radiation by relativistic dipoles. II 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment Gushchina, V. S. aut Zhukova, I. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 3 vom: März, Seite 247-252 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:3 month:03 pages:247-252 https://doi.org/10.1007/BF00559629 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 3 03 247-252
spelling	10.1007/BF00559629 doi (DE-627)OLC2033040453 (DE-He213)BF00559629-p DE-627 ger DE-627 rakwb eng 530 370 VZ Bordovitsyn, V. A. verfasserin aut Radiation by relativistic dipoles. II 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment Gushchina, V. S. aut Zhukova, I. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 3 vom: März, Seite 247-252 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:3 month:03 pages:247-252 https://doi.org/10.1007/BF00559629 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 3 03 247-252
allfields_unstemmed	10.1007/BF00559629 doi (DE-627)OLC2033040453 (DE-He213)BF00559629-p DE-627 ger DE-627 rakwb eng 530 370 VZ Bordovitsyn, V. A. verfasserin aut Radiation by relativistic dipoles. II 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment Gushchina, V. S. aut Zhukova, I. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 3 vom: März, Seite 247-252 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:3 month:03 pages:247-252 https://doi.org/10.1007/BF00559629 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 3 03 247-252
allfieldsGer	10.1007/BF00559629 doi (DE-627)OLC2033040453 (DE-He213)BF00559629-p DE-627 ger DE-627 rakwb eng 530 370 VZ Bordovitsyn, V. A. verfasserin aut Radiation by relativistic dipoles. II 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment Gushchina, V. S. aut Zhukova, I. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 3 vom: März, Seite 247-252 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:3 month:03 pages:247-252 https://doi.org/10.1007/BF00559629 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 3 03 247-252
allfieldsSound	10.1007/BF00559629 doi (DE-627)OLC2033040453 (DE-He213)BF00559629-p DE-627 ger DE-627 rakwb eng 530 370 VZ Bordovitsyn, V. A. verfasserin aut Radiation by relativistic dipoles. II 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. Dipole Moment Electromagnetic Field Magnetic Dipole Rest Frame Electric Dipole Moment Gushchina, V. S. aut Zhukova, I. N. aut Enthalten in Russian physics journal Kluwer Academic Publishers-Plenum Publishers, 1992 36(1993), 3 vom: März, Seite 247-252 (DE-627)131169718 (DE-600)1138228-4 (DE-576)033029253 1064-8887 nnns volume:36 year:1993 number:3 month:03 pages:247-252 https://doi.org/10.1007/BF00559629 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_32 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2021 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4700 AR 36 1993 3 03 247-252
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abstract	Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. © Plenum Publishing Corporation 1993
abstractGer	Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. © Plenum Publishing Corporation 1993
abstract_unstemmed	Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed. © Plenum Publishing Corporation 1993
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A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Radiation by relativistic dipoles. II</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1993</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Plenum Publishing Corporation 1993</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In a continuation of an earlier study, the electromagnetic fields of a point magnetic moment — a magneton — in uniform rectilinear motion, with a given spin precession, are analyzed. It is shown that the same equations can be found through Lorentz transformations from the corresponding expressions in the rest frame. The relationship between the electric and magnetic fieldsE andH radiated by a point magnetic dipole moment μ and a point electric dipole moment ν is derived through the use of dual transformations of the electromagnetic field tensor. It is assumed that each moment is in relativistic and otherwise arbitrary motion. In the relativistic case, as in the nonrelativistic case, the switch μ→ν is accompanied by the replacementsH→E, E→-H. A covariant formalism is developed for describing the electromagnetic fields in the wave zone. The electromagnetic field tensor associated with the radiation is analyzed.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Dipole Moment</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Electromagnetic Field</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Magnetic Dipole</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Rest Frame</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Electric Dipole Moment</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gushchina, V. S.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zhukova, I. 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Radiation by relativistic dipoles. II

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