Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture
Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in te...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Lipatnikov, A. N. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1993 |
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| Schlagwörter: |
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| Anmerkung: |
© Plenum Publishing Corporation 1993 |
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| Übergeordnetes Werk: |
Enthalten in: Combustion, explosion and shock waves - Kluwer Academic Publishers-Plenum Publishers, 1966, 29(1993), 3 vom: Mai, Seite 326-330 |
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| Übergeordnetes Werk: |
volume:29 ; year:1993 ; number:3 ; month:05 ; pages:326-330 |
| Links: |
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| DOI / URN: |
10.1007/BF00797651 |
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| Katalog-ID: |
OLC2072164125 |
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| 520 | |a Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. | ||
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10.1007/BF00797651 doi (DE-627)OLC2072164125 (DE-He213)BF00797651-p DE-627 ger DE-627 rakwb eng 660 VZ Lipatnikov, A. N. verfasserin aut Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. Oxygen Radiation Combustion Oxygen Atom Numerical Modeling Enthalten in Combustion, explosion and shock waves Kluwer Academic Publishers-Plenum Publishers, 1966 29(1993), 3 vom: Mai, Seite 326-330 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:29 year:1993 number:3 month:05 pages:326-330 https://doi.org/10.1007/BF00797651 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_4082 GBV_ILN_4700 AR 29 1993 3 05 326-330 |
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10.1007/BF00797651 doi (DE-627)OLC2072164125 (DE-He213)BF00797651-p DE-627 ger DE-627 rakwb eng 660 VZ Lipatnikov, A. N. verfasserin aut Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. Oxygen Radiation Combustion Oxygen Atom Numerical Modeling Enthalten in Combustion, explosion and shock waves Kluwer Academic Publishers-Plenum Publishers, 1966 29(1993), 3 vom: Mai, Seite 326-330 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:29 year:1993 number:3 month:05 pages:326-330 https://doi.org/10.1007/BF00797651 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_4082 GBV_ILN_4700 AR 29 1993 3 05 326-330 |
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10.1007/BF00797651 doi (DE-627)OLC2072164125 (DE-He213)BF00797651-p DE-627 ger DE-627 rakwb eng 660 VZ Lipatnikov, A. N. verfasserin aut Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. Oxygen Radiation Combustion Oxygen Atom Numerical Modeling Enthalten in Combustion, explosion and shock waves Kluwer Academic Publishers-Plenum Publishers, 1966 29(1993), 3 vom: Mai, Seite 326-330 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:29 year:1993 number:3 month:05 pages:326-330 https://doi.org/10.1007/BF00797651 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_4082 GBV_ILN_4700 AR 29 1993 3 05 326-330 |
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10.1007/BF00797651 doi (DE-627)OLC2072164125 (DE-He213)BF00797651-p DE-627 ger DE-627 rakwb eng 660 VZ Lipatnikov, A. N. verfasserin aut Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. Oxygen Radiation Combustion Oxygen Atom Numerical Modeling Enthalten in Combustion, explosion and shock waves Kluwer Academic Publishers-Plenum Publishers, 1966 29(1993), 3 vom: Mai, Seite 326-330 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:29 year:1993 number:3 month:05 pages:326-330 https://doi.org/10.1007/BF00797651 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_4082 GBV_ILN_4700 AR 29 1993 3 05 326-330 |
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10.1007/BF00797651 doi (DE-627)OLC2072164125 (DE-He213)BF00797651-p DE-627 ger DE-627 rakwb eng 660 VZ Lipatnikov, A. N. verfasserin aut Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture 1993 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1993 Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. Oxygen Radiation Combustion Oxygen Atom Numerical Modeling Enthalten in Combustion, explosion and shock waves Kluwer Academic Publishers-Plenum Publishers, 1966 29(1993), 3 vom: Mai, Seite 326-330 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:29 year:1993 number:3 month:05 pages:326-330 https://doi.org/10.1007/BF00797651 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_4082 GBV_ILN_4700 AR 29 1993 3 05 326-330 |
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Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture |
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Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. © Plenum Publishing Corporation 1993 |
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Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. © Plenum Publishing Corporation 1993 |
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Abstract Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation. © Plenum Publishing Corporation 1993 |
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Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture |
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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">OLC2072164125</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503022607.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1993 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF00797651</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2072164125</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF00797651-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">Lipatnikov, A. N.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Numerical modeling of nitrogen oxide formation in turbulent combustion of a premixed gas mixture</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 Based on the particle equilibrium approximation and introducing a prespecified probability density function of the bimodal type, we have developed a method for calculation of the rate of NO formation in turbulent combustion of a premixed gas mixture, taking into account the pulsations in temperature and composition caused by the chaotic motion of the thin reaction zone, the superequilibrium concentration of oxygen atoms, and the energy losses to radiation. Based on the numerical results, we have compared the effects of the listed factors on the rate of nitrogen oxide formation.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Oxygen</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Radiation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Combustion</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Oxygen Atom</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Numerical Modeling</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">Kluwer Academic Publishers-Plenum Publishers, 1966</subfield><subfield code="g">29(1993), 3 vom: Mai, Seite 326-330</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:29</subfield><subfield code="g">year:1993</subfield><subfield code="g">number:3</subfield><subfield code="g">month:05</subfield><subfield code="g">pages:326-330</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF00797651</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_4082</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">29</subfield><subfield code="j">1993</subfield><subfield code="e">3</subfield><subfield code="c">05</subfield><subfield code="h">326-330</subfield></datafield></record></collection>
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