Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen
Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. C...
Ausführliche Beschreibung
Autor*in: |
Shtertser, A. A. [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2022 |
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Schlagwörter: |
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Anmerkung: |
© Pleiades Publishing, Ltd. 2022 |
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Übergeordnetes Werk: |
Enthalten in: Combustion, explosion and shock waves - New York, NY [u.a.] : Consultants Bureau, 1966, 58(2022), 6 vom: Dez., Seite 709-718 |
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Übergeordnetes Werk: |
volume:58 ; year:2022 ; number:6 ; month:12 ; pages:709-718 |
Links: |
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DOI / URN: |
10.1134/S0010508222060089 |
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Katalog-ID: |
SPR051322196 |
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520 | |a Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. | ||
650 | 4 | |a pulse gas detonation device |7 (dpeaa)DE-He213 | |
650 | 4 | |a acetylene–oxygen mixture |7 (dpeaa)DE-He213 | |
650 | 4 | |a detonation initiation |7 (dpeaa)DE-He213 | |
650 | 4 | |a cell size |7 (dpeaa)DE-He213 | |
650 | 4 | |a reaction products |7 (dpeaa)DE-He213 | |
650 | 4 | |a booster charge |7 (dpeaa)DE-He213 | |
650 | 4 | |a hydrogen |7 (dpeaa)DE-He213 | |
650 | 4 | |a nanosized detonation carbon |7 (dpeaa)DE-He213 | |
650 | 4 | |a carbon footprint |7 (dpeaa)DE-He213 | |
700 | 1 | |a Ul’yanitskii, V. Yu. |4 aut | |
700 | 1 | |a Rybin, D. K. |4 aut | |
700 | 1 | |a Batraev, I. S. |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Combustion, explosion and shock waves |d New York, NY [u.a.] : Consultants Bureau, 1966 |g 58(2022), 6 vom: Dez., Seite 709-718 |w (DE-627)325568626 |w (DE-600)2037134-2 |x 1573-8345 |7 nnns |
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10.1134/S0010508222060089 doi (DE-627)SPR051322196 (SPR)S0010508222060089-e DE-627 ger DE-627 rakwb eng Shtertser, A. A. verfasserin aut Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 Ul’yanitskii, V. Yu. aut Rybin, D. K. aut Batraev, I. S. aut Enthalten in Combustion, explosion and shock waves New York, NY [u.a.] : Consultants Bureau, 1966 58(2022), 6 vom: Dez., Seite 709-718 (DE-627)325568626 (DE-600)2037134-2 1573-8345 nnns volume:58 year:2022 number:6 month:12 pages:709-718 https://dx.doi.org/10.1134/S0010508222060089 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 58 2022 6 12 709-718 |
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10.1134/S0010508222060089 doi (DE-627)SPR051322196 (SPR)S0010508222060089-e DE-627 ger DE-627 rakwb eng Shtertser, A. A. verfasserin aut Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 Ul’yanitskii, V. Yu. aut Rybin, D. K. aut Batraev, I. S. aut Enthalten in Combustion, explosion and shock waves New York, NY [u.a.] : Consultants Bureau, 1966 58(2022), 6 vom: Dez., Seite 709-718 (DE-627)325568626 (DE-600)2037134-2 1573-8345 nnns volume:58 year:2022 number:6 month:12 pages:709-718 https://dx.doi.org/10.1134/S0010508222060089 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 58 2022 6 12 709-718 |
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10.1134/S0010508222060089 doi (DE-627)SPR051322196 (SPR)S0010508222060089-e DE-627 ger DE-627 rakwb eng Shtertser, A. A. verfasserin aut Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 Ul’yanitskii, V. Yu. aut Rybin, D. K. aut Batraev, I. S. aut Enthalten in Combustion, explosion and shock waves New York, NY [u.a.] : Consultants Bureau, 1966 58(2022), 6 vom: Dez., Seite 709-718 (DE-627)325568626 (DE-600)2037134-2 1573-8345 nnns volume:58 year:2022 number:6 month:12 pages:709-718 https://dx.doi.org/10.1134/S0010508222060089 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 58 2022 6 12 709-718 |
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10.1134/S0010508222060089 doi (DE-627)SPR051322196 (SPR)S0010508222060089-e DE-627 ger DE-627 rakwb eng Shtertser, A. A. verfasserin aut Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 Ul’yanitskii, V. Yu. aut Rybin, D. K. aut Batraev, I. S. aut Enthalten in Combustion, explosion and shock waves New York, NY [u.a.] : Consultants Bureau, 1966 58(2022), 6 vom: Dez., Seite 709-718 (DE-627)325568626 (DE-600)2037134-2 1573-8345 nnns volume:58 year:2022 number:6 month:12 pages:709-718 https://dx.doi.org/10.1134/S0010508222060089 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 58 2022 6 12 709-718 |
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10.1134/S0010508222060089 doi (DE-627)SPR051322196 (SPR)S0010508222060089-e DE-627 ger DE-627 rakwb eng Shtertser, A. A. verfasserin aut Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 Ul’yanitskii, V. Yu. aut Rybin, D. K. aut Batraev, I. S. aut Enthalten in Combustion, explosion and shock waves New York, NY [u.a.] : Consultants Bureau, 1966 58(2022), 6 vom: Dez., Seite 709-718 (DE-627)325568626 (DE-600)2037134-2 1573-8345 nnns volume:58 year:2022 number:6 month:12 pages:709-718 https://dx.doi.org/10.1134/S0010508222060089 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 58 2022 6 12 709-718 |
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English |
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Enthalten in Combustion, explosion and shock waves 58(2022), 6 vom: Dez., Seite 709-718 volume:58 year:2022 number:6 month:12 pages:709-718 |
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Enthalten in Combustion, explosion and shock waves 58(2022), 6 vom: Dez., Seite 709-718 volume:58 year:2022 number:6 month:12 pages:709-718 |
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pulse gas detonation device acetylene–oxygen mixture detonation initiation cell size reaction products booster charge hydrogen nanosized detonation carbon carbon footprint |
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Combustion, explosion and shock waves |
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Shtertser, A. A. @@aut@@ Ul’yanitskii, V. Yu. @@aut@@ Rybin, D. K. @@aut@@ Batraev, I. S. @@aut@@ |
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A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Pleiades Publishing, Ltd. 2022</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. 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author |
Shtertser, A. A. |
spellingShingle |
Shtertser, A. A. misc pulse gas detonation device misc acetylene–oxygen mixture misc detonation initiation misc cell size misc reaction products misc booster charge misc hydrogen misc nanosized detonation carbon misc carbon footprint Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen |
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topic_title |
Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen pulse gas detonation device (dpeaa)DE-He213 acetylene–oxygen mixture (dpeaa)DE-He213 detonation initiation (dpeaa)DE-He213 cell size (dpeaa)DE-He213 reaction products (dpeaa)DE-He213 booster charge (dpeaa)DE-He213 hydrogen (dpeaa)DE-He213 nanosized detonation carbon (dpeaa)DE-He213 carbon footprint (dpeaa)DE-He213 |
topic |
misc pulse gas detonation device misc acetylene–oxygen mixture misc detonation initiation misc cell size misc reaction products misc booster charge misc hydrogen misc nanosized detonation carbon misc carbon footprint |
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misc pulse gas detonation device misc acetylene–oxygen mixture misc detonation initiation misc cell size misc reaction products misc booster charge misc hydrogen misc nanosized detonation carbon misc carbon footprint |
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misc pulse gas detonation device misc acetylene–oxygen mixture misc detonation initiation misc cell size misc reaction products misc booster charge misc hydrogen misc nanosized detonation carbon misc carbon footprint |
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Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen |
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title_full |
Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen |
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Shtertser, A. A. |
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Combustion, explosion and shock waves |
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Shtertser, A. A. Ul’yanitskii, V. Yu. Rybin, D. K. Batraev, I. S. |
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Elektronische Aufsätze |
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Shtertser, A. A. |
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10.1134/S0010508222060089 |
title_sort |
detonation decomposition of acetylene at atmospheric pressure in the presence of small additives of oxygen |
title_auth |
Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen |
abstract |
Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. © Pleiades Publishing, Ltd. 2022 |
abstractGer |
Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. © Pleiades Publishing, Ltd. 2022 |
abstract_unstemmed |
Abstract A pulse gas-detonation device (PGDD) is applied to investigate the process of initiation and detonation in $ C_{2} %$ H_{2} $+%$k%%$ O_{2} $ acetylene–oxygen mixtures, including those with a low oxygen content near the upper detonation concentration limit, at initial atmospheric pressure. Cell sizes, detonation velocities, and pressures in detonation products are measured in a range of %$k%$ from zero to unity. The detonation product composition is calculated. Upper detonation limits in the PGDD barrels with diameters of 14, 26, 46, and 104 mm are determined. The volume of booster charges required to initiate detonation in the limiting modes are revealed. As for the hydrogen energy industry, the methane %$\to%$ acetylene %$\to%$ hydrogen + nanosized detonation carbon technological chain is considered, and the characteristics of the PGDD as a hydrogen generator are estimated. © Pleiades Publishing, Ltd. 2022 |
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title_short |
Detonation Decomposition of Acetylene at Atmospheric Pressure in the Presence of Small Additives of Oxygen |
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https://dx.doi.org/10.1134/S0010508222060089 |
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Ul’yanitskii, V. Yu Rybin, D. K. Batraev, I. S. |
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Ul’yanitskii, V. Yu Rybin, D. K. Batraev, I. S. |
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10.1134/S0010508222060089 |
up_date |
2024-07-03T21:07:34.404Z |
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score |
7.3994675 |