Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam
Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case und...
Ausführliche Beschreibung
Autor*in: |
Kolesnikov, E. K. [verfasserIn] |
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Format: |
Artikel |
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Sprache: |
Englisch |
Erschienen: |
2002 |
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Schlagwörter: |
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Anmerkung: |
© MAIK "Nauka/Interperiodica" 2002 |
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Übergeordnetes Werk: |
Enthalten in: Plasma physics reports - Nauka/Interperiodica, 1993, 28(2002), 4 vom: Apr., Seite 327-334 |
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Übergeordnetes Werk: |
volume:28 ; year:2002 ; number:4 ; month:04 ; pages:327-334 |
Links: |
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DOI / URN: |
10.1134/1.1469173 |
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Katalog-ID: |
OLC2071100476 |
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520 | |a Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. | ||
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650 | 4 | |a Negative Charge | |
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650 | 4 | |a Field Potential | |
650 | 4 | |a Outer Region | |
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10.1134/1.1469173 doi (DE-627)OLC2071100476 (DE-He213)1.1469173-p DE-627 ger DE-627 rakwb eng 530 VZ Kolesnikov, E. K. verfasserin aut Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. Electron Beam Negative Charge Space Charge Field Potential Outer Region Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 4 vom: Apr., Seite 327-334 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:4 month:04 pages:327-334 https://doi.org/10.1134/1.1469173 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 AR 28 2002 4 04 327-334 |
spelling |
10.1134/1.1469173 doi (DE-627)OLC2071100476 (DE-He213)1.1469173-p DE-627 ger DE-627 rakwb eng 530 VZ Kolesnikov, E. K. verfasserin aut Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. Electron Beam Negative Charge Space Charge Field Potential Outer Region Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 4 vom: Apr., Seite 327-334 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:4 month:04 pages:327-334 https://doi.org/10.1134/1.1469173 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 AR 28 2002 4 04 327-334 |
allfields_unstemmed |
10.1134/1.1469173 doi (DE-627)OLC2071100476 (DE-He213)1.1469173-p DE-627 ger DE-627 rakwb eng 530 VZ Kolesnikov, E. K. verfasserin aut Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. Electron Beam Negative Charge Space Charge Field Potential Outer Region Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 4 vom: Apr., Seite 327-334 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:4 month:04 pages:327-334 https://doi.org/10.1134/1.1469173 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 AR 28 2002 4 04 327-334 |
allfieldsGer |
10.1134/1.1469173 doi (DE-627)OLC2071100476 (DE-He213)1.1469173-p DE-627 ger DE-627 rakwb eng 530 VZ Kolesnikov, E. K. verfasserin aut Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. Electron Beam Negative Charge Space Charge Field Potential Outer Region Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 4 vom: Apr., Seite 327-334 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:4 month:04 pages:327-334 https://doi.org/10.1134/1.1469173 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 AR 28 2002 4 04 327-334 |
allfieldsSound |
10.1134/1.1469173 doi (DE-627)OLC2071100476 (DE-He213)1.1469173-p DE-627 ger DE-627 rakwb eng 530 VZ Kolesnikov, E. K. verfasserin aut Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. Electron Beam Negative Charge Space Charge Field Potential Outer Region Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 4 vom: Apr., Seite 327-334 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:4 month:04 pages:327-334 https://doi.org/10.1134/1.1469173 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_2014 GBV_ILN_4323 AR 28 2002 4 04 327-334 |
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Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. © MAIK "Nauka/Interperiodica" 2002 |
abstractGer |
Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. © MAIK "Nauka/Interperiodica" 2002 |
abstract_unstemmed |
Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions. © MAIK "Nauka/Interperiodica" 2002 |
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K.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Calculation of the electric field in space plasma near a conducting sphere injecting an electron beam</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2002</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">© MAIK "Nauka/Interperiodica" 2002</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The problem is considered of determining the electric field induced in the vicinity of a conducting spherical body that is at rest in a collisionless plasma and at the surface of which there is a prescribed sink of negative charge. The problem is solved for the general relativistic case under the assumption that the electron velocity in the neutralizing current is comparable with the speed of light. An integrodifferential equation is derived that describes the radial behavior of the electric field potential in the vicinity of the injector. A simplified method for determining the potential in the perturbed region is developed. The method implies that the problems of the potentials in a space charge region of radius R* (with a prescribed boundary potential ϕ*) adjacent the body and in the outer region r>R* are solved separately and then the solutions obtained are matched at boundary between these regions.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Electron Beam</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Negative Charge</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Space Charge</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Field Potential</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Outer Region</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Plasma physics reports</subfield><subfield code="d">Nauka/Interperiodica, 1993</subfield><subfield code="g">28(2002), 4 vom: Apr., Seite 327-334</subfield><subfield code="w">(DE-627)171253191</subfield><subfield code="w">(DE-600)1170407-X</subfield><subfield code="w">(DE-576)03886956X</subfield><subfield code="x">1063-780X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:28</subfield><subfield code="g">year:2002</subfield><subfield code="g">number:4</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:327-334</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.1469173</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">28</subfield><subfield code="j">2002</subfield><subfield code="e">4</subfield><subfield code="c">04</subfield><subfield code="h">327-334</subfield></datafield></record></collection>
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