MHD simulations of molybdenum X-pinches
Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geomet...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Ivanenkov, G. V. [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), 10 vom: Okt., Seite 814-826 |
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| Übergeordnetes Werk: |
volume:28 ; year:2002 ; number:10 ; month:10 ; pages:814-826 |
| Links: |
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| DOI / URN: |
10.1134/1.1513835 |
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| Katalog-ID: |
OLC2071101154 |
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| 520 | |a Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. | ||
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10.1134/1.1513835 doi (DE-627)OLC2071101154 (DE-He213)1.1513835-p DE-627 ger DE-627 rakwb eng 530 VZ Ivanenkov, G. V. verfasserin aut MHD simulations of molybdenum X-pinches 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. Shock Wave Molybdenum Large Masse Actual Discharge Initial Geometry Stepniewski, W. aut Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 10 vom: Okt., Seite 814-826 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:10 month:10 pages:814-826 https://doi.org/10.1134/1.1513835 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 10 10 814-826 |
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10.1134/1.1513835 doi (DE-627)OLC2071101154 (DE-He213)1.1513835-p DE-627 ger DE-627 rakwb eng 530 VZ Ivanenkov, G. V. verfasserin aut MHD simulations of molybdenum X-pinches 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. Shock Wave Molybdenum Large Masse Actual Discharge Initial Geometry Stepniewski, W. aut Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 10 vom: Okt., Seite 814-826 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:10 month:10 pages:814-826 https://doi.org/10.1134/1.1513835 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 10 10 814-826 |
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10.1134/1.1513835 doi (DE-627)OLC2071101154 (DE-He213)1.1513835-p DE-627 ger DE-627 rakwb eng 530 VZ Ivanenkov, G. V. verfasserin aut MHD simulations of molybdenum X-pinches 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. Shock Wave Molybdenum Large Masse Actual Discharge Initial Geometry Stepniewski, W. aut Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 10 vom: Okt., Seite 814-826 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:10 month:10 pages:814-826 https://doi.org/10.1134/1.1513835 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 10 10 814-826 |
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10.1134/1.1513835 doi (DE-627)OLC2071101154 (DE-He213)1.1513835-p DE-627 ger DE-627 rakwb eng 530 VZ Ivanenkov, G. V. verfasserin aut MHD simulations of molybdenum X-pinches 2002 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK "Nauka/Interperiodica" 2002 Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. Shock Wave Molybdenum Large Masse Actual Discharge Initial Geometry Stepniewski, W. aut Enthalten in Plasma physics reports Nauka/Interperiodica, 1993 28(2002), 10 vom: Okt., Seite 814-826 (DE-627)171253191 (DE-600)1170407-X (DE-576)03886956X 1063-780X nnns volume:28 year:2002 number:10 month:10 pages:814-826 https://doi.org/10.1134/1.1513835 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 10 10 814-826 |
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Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. © MAIK "Nauka/Interperiodica" 2002 |
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Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. © MAIK "Nauka/Interperiodica" 2002 |
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Abstract The compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction. © MAIK "Nauka/Interperiodica" 2002 |
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V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">MHD simulations of molybdenum X-pinches</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 compression of molybdenum X-pinches with paraboloidal and conical initial geometries is investigated using numerical radiative MHD models. The model with conical initial geometry provides a more complete description of the axial plasma motion, better reflects the actual discharge geometry, and applies to molybdenum loads with larger masses. Both models make it possible to describe the main compression stages, including the formation of a “minidiode,” the formation of a narrow neck in the constriction, the microexplosion of a “hot spot,” and the generation of shock waves followed by the breaking of the constriction.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Shock Wave</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Molybdenum</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Large Masse</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Actual Discharge</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Initial Geometry</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Stepniewski, W.</subfield><subfield code="4">aut</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), 10 vom: Okt., Seite 814-826</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:10</subfield><subfield code="g">month:10</subfield><subfield code="g">pages:814-826</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.1513835</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">10</subfield><subfield code="c">10</subfield><subfield code="h">814-826</subfield></datafield></record></collection>
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