Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space
Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plas...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Mann, D. S. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1979 |
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| Schlagwörter: |
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| Anmerkung: |
© D. Reidel Publishing Co. 1979 |
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| Übergeordnetes Werk: |
Enthalten in: Astrophysics and space science - Kluwer Academic Publishers, 1968, 63(1979), 2 vom: Juli, Seite 405-417 |
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| Übergeordnetes Werk: |
volume:63 ; year:1979 ; number:2 ; month:07 ; pages:405-417 |
| Links: |
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| DOI / URN: |
10.1007/BF00638911 |
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| Katalog-ID: |
OLC2066136107 |
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| 245 | 1 | 0 | |a Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space |
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| 520 | |a Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. | ||
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| 650 | 4 | |a Anisotropy | |
| 650 | 4 | |a Electromagnetic Radiation | |
| 650 | 4 | |a Radiation Field | |
| 650 | 4 | |a Radiation Pattern | |
| 700 | 1 | |a Mukherjee, P. K. |4 aut | |
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10.1007/BF00638911 doi (DE-627)OLC2066136107 (DE-He213)BF00638911-p DE-627 ger DE-627 rakwb eng 520 530 620 VZ 16,12 ssgn Mann, D. S. verfasserin aut Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space 1979 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Co. 1979 Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. Radiation Anisotropy Electromagnetic Radiation Radiation Field Radiation Pattern Mukherjee, P. K. aut Enthalten in Astrophysics and space science Kluwer Academic Publishers, 1968 63(1979), 2 vom: Juli, Seite 405-417 (DE-627)129062723 (DE-600)629-4 (DE-576)014393522 0004-640X nnns volume:63 year:1979 number:2 month:07 pages:405-417 https://doi.org/10.1007/BF00638911 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_31 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4700 AR 63 1979 2 07 405-417 |
| spelling |
10.1007/BF00638911 doi (DE-627)OLC2066136107 (DE-He213)BF00638911-p DE-627 ger DE-627 rakwb eng 520 530 620 VZ 16,12 ssgn Mann, D. S. verfasserin aut Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space 1979 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Co. 1979 Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. Radiation Anisotropy Electromagnetic Radiation Radiation Field Radiation Pattern Mukherjee, P. K. aut Enthalten in Astrophysics and space science Kluwer Academic Publishers, 1968 63(1979), 2 vom: Juli, Seite 405-417 (DE-627)129062723 (DE-600)629-4 (DE-576)014393522 0004-640X nnns volume:63 year:1979 number:2 month:07 pages:405-417 https://doi.org/10.1007/BF00638911 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_31 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4700 AR 63 1979 2 07 405-417 |
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10.1007/BF00638911 doi (DE-627)OLC2066136107 (DE-He213)BF00638911-p DE-627 ger DE-627 rakwb eng 520 530 620 VZ 16,12 ssgn Mann, D. S. verfasserin aut Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space 1979 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Co. 1979 Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. Radiation Anisotropy Electromagnetic Radiation Radiation Field Radiation Pattern Mukherjee, P. K. aut Enthalten in Astrophysics and space science Kluwer Academic Publishers, 1968 63(1979), 2 vom: Juli, Seite 405-417 (DE-627)129062723 (DE-600)629-4 (DE-576)014393522 0004-640X nnns volume:63 year:1979 number:2 month:07 pages:405-417 https://doi.org/10.1007/BF00638911 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_31 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4700 AR 63 1979 2 07 405-417 |
| allfieldsGer |
10.1007/BF00638911 doi (DE-627)OLC2066136107 (DE-He213)BF00638911-p DE-627 ger DE-627 rakwb eng 520 530 620 VZ 16,12 ssgn Mann, D. S. verfasserin aut Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space 1979 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Co. 1979 Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. Radiation Anisotropy Electromagnetic Radiation Radiation Field Radiation Pattern Mukherjee, P. K. aut Enthalten in Astrophysics and space science Kluwer Academic Publishers, 1968 63(1979), 2 vom: Juli, Seite 405-417 (DE-627)129062723 (DE-600)629-4 (DE-576)014393522 0004-640X nnns volume:63 year:1979 number:2 month:07 pages:405-417 https://doi.org/10.1007/BF00638911 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_31 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4700 AR 63 1979 2 07 405-417 |
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10.1007/BF00638911 doi (DE-627)OLC2066136107 (DE-He213)BF00638911-p DE-627 ger DE-627 rakwb eng 520 530 620 VZ 16,12 ssgn Mann, D. S. verfasserin aut Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space 1979 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Co. 1979 Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. Radiation Anisotropy Electromagnetic Radiation Radiation Field Radiation Pattern Mukherjee, P. K. aut Enthalten in Astrophysics and space science Kluwer Academic Publishers, 1968 63(1979), 2 vom: Juli, Seite 405-417 (DE-627)129062723 (DE-600)629-4 (DE-576)014393522 0004-640X nnns volume:63 year:1979 number:2 month:07 pages:405-417 https://doi.org/10.1007/BF00638911 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_31 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4700 AR 63 1979 2 07 405-417 |
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Enthalten in Astrophysics and space science 63(1979), 2 vom: Juli, Seite 405-417 volume:63 year:1979 number:2 month:07 pages:405-417 |
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Enthalten in Astrophysics and space science 63(1979), 2 vom: Juli, Seite 405-417 volume:63 year:1979 number:2 month:07 pages:405-417 |
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Electromagnetic radiation from line sources interacting with a moving uniaxial dielectric or plasma half-space |
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Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. © D. Reidel Publishing Co. 1979 |
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Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. © D. Reidel Publishing Co. 1979 |
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Abstract The problem of electromagnetic radiation from electric and magnetic line sources interacting with a moving uniaxially anisotropic dielectric or plasma half-space is treated. The anisotropy of the plasma is due to an infinitely strong magnetizing field impressedparallel to the motion of plasma. The line source is oriented normal to the direction of medium motion. TheE and theH modes are excited independently in the medium by the magnetic and the electric line sources, respectively. Invoking the saddle-point method of integration, the far-zone radiation field and the radiation pattern are obtained for both line sources. It is found that the radiation from an electric line source is not affected by the anisotropy of the moving medium and that a magnetic line source invacuum has finite components of radiation in directions which are parallel and antiparallel to the direction of motion, for the case of a uniaxial plasma in contrast to the results for a uniaxial dielectric. Numerical results for the far-zone radiation pattern, referring to a magnetic line source, are presented for several values of parameters characterizing the non-dimensional velocity, the anisotropy of the medium, the electron-plasma density and the location of the line source. © D. Reidel Publishing Co. 1979 |
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