Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field
Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree mat...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bichenkov, E. I. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1997 |
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| Schlagwörter: |
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| Anmerkung: |
© Plenum Publishing Corporation 1998 |
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| Übergeordnetes Werk: |
Enthalten in: Combustion, explosion and shock waves - Springer US, 1966, 33(1997), 4 vom: Juli, Seite 491-503 |
|---|---|
| Übergeordnetes Werk: |
volume:33 ; year:1997 ; number:4 ; month:07 ; pages:491-503 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF02671844 |
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OLC2072169313 |
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| 520 | |a Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. | ||
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10.1007/BF02671844 doi (DE-627)OLC2072169313 (DE-He213)BF02671844-p DE-627 ger DE-627 rakwb eng 660 VZ Bichenkov, E. I. verfasserin aut Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1998 Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. Diffusion Zone Shock Wave Front Transverse Magnetic Field Oscillation Zone Oscillation Component Enthalten in Combustion, explosion and shock waves Springer US, 1966 33(1997), 4 vom: Juli, Seite 491-503 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:33 year:1997 number:4 month:07 pages:491-503 https://doi.org/10.1007/BF02671844 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_70 GBV_ILN_4027 GBV_ILN_4700 AR 33 1997 4 07 491-503 |
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10.1007/BF02671844 doi (DE-627)OLC2072169313 (DE-He213)BF02671844-p DE-627 ger DE-627 rakwb eng 660 VZ Bichenkov, E. I. verfasserin aut Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1998 Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. Diffusion Zone Shock Wave Front Transverse Magnetic Field Oscillation Zone Oscillation Component Enthalten in Combustion, explosion and shock waves Springer US, 1966 33(1997), 4 vom: Juli, Seite 491-503 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:33 year:1997 number:4 month:07 pages:491-503 https://doi.org/10.1007/BF02671844 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_70 GBV_ILN_4027 GBV_ILN_4700 AR 33 1997 4 07 491-503 |
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10.1007/BF02671844 doi (DE-627)OLC2072169313 (DE-He213)BF02671844-p DE-627 ger DE-627 rakwb eng 660 VZ Bichenkov, E. I. verfasserin aut Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1998 Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. Diffusion Zone Shock Wave Front Transverse Magnetic Field Oscillation Zone Oscillation Component Enthalten in Combustion, explosion and shock waves Springer US, 1966 33(1997), 4 vom: Juli, Seite 491-503 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:33 year:1997 number:4 month:07 pages:491-503 https://doi.org/10.1007/BF02671844 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_70 GBV_ILN_4027 GBV_ILN_4700 AR 33 1997 4 07 491-503 |
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10.1007/BF02671844 doi (DE-627)OLC2072169313 (DE-He213)BF02671844-p DE-627 ger DE-627 rakwb eng 660 VZ Bichenkov, E. I. verfasserin aut Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1998 Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. Diffusion Zone Shock Wave Front Transverse Magnetic Field Oscillation Zone Oscillation Component Enthalten in Combustion, explosion and shock waves Springer US, 1966 33(1997), 4 vom: Juli, Seite 491-503 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:33 year:1997 number:4 month:07 pages:491-503 https://doi.org/10.1007/BF02671844 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_70 GBV_ILN_4027 GBV_ILN_4700 AR 33 1997 4 07 491-503 |
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10.1007/BF02671844 doi (DE-627)OLC2072169313 (DE-He213)BF02671844-p DE-627 ger DE-627 rakwb eng 660 VZ Bichenkov, E. I. verfasserin aut Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1998 Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. Diffusion Zone Shock Wave Front Transverse Magnetic Field Oscillation Zone Oscillation Component Enthalten in Combustion, explosion and shock waves Springer US, 1966 33(1997), 4 vom: Juli, Seite 491-503 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:33 year:1997 number:4 month:07 pages:491-503 https://doi.org/10.1007/BF02671844 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE GBV_ILN_70 GBV_ILN_4027 GBV_ILN_4700 AR 33 1997 4 07 491-503 |
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Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field |
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Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. © Plenum Publishing Corporation 1998 |
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Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. © Plenum Publishing Corporation 1998 |
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Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front. © Plenum Publishing Corporation 1998 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2072169313</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503022625.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1997 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02671844</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2072169313</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02671844-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">660</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Bichenkov, E. I.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Structure of a shock-induced stationary current wave in a conducting material with a transverse magnetic field</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1997</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 1998</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this paper, a two-fluid model of a plane stationary shock wave in a conductor is proposed, and the current structure of the wave is considered. For an ideal hydrodynamic discontinuity, it is shown that the field and current distributions consists of a wide diffusion zone of shockfree material and a small-scale zone of high-frequency oscillations related to relaxation of the electron density to the ion density. The structure of the oscillation zone is considered with variation in the properties of the material and with possible variation in the electric conductivity in the shock wave. The time required for the attainment of an equilibrium density of charges is calculated. It is shown that, for conducting materials, the shock-induced current is determined by compressibility and is almost entirely concentrated in the diffusion zone. The width of this zone is determined by the electric conductivity of the material in the initial state and does not depend on the properties of the material behind the wave front.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Diffusion Zone</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Shock Wave Front</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Transverse Magnetic Field</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Oscillation Zone</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Oscillation Component</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Combustion, explosion and shock waves</subfield><subfield code="d">Springer US, 1966</subfield><subfield code="g">33(1997), 4 vom: Juli, Seite 491-503</subfield><subfield code="w">(DE-627)12959282X</subfield><subfield code="w">(DE-600)240334-1</subfield><subfield code="w">(DE-576)015085570</subfield><subfield code="x">0010-5082</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:33</subfield><subfield code="g">year:1997</subfield><subfield code="g">number:4</subfield><subfield code="g">month:07</subfield><subfield code="g">pages:491-503</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02671844</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-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-CHE</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_4027</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">33</subfield><subfield code="j">1997</subfield><subfield code="e">4</subfield><subfield code="c">07</subfield><subfield code="h">491-503</subfield></datafield></record></collection>
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