Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF
Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled w...
Ausführliche Beschreibung
Autor*in: |
Sharaborin, D. K. [verfasserIn] |
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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 - Pleiades Publishing, 1966, 58(2022), 5 vom: Okt., Seite 507-515 |
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Übergeordnetes Werk: |
volume:58 ; year:2022 ; number:5 ; month:10 ; pages:507-515 |
Links: |
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DOI / URN: |
10.1134/S001050822205001X |
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Katalog-ID: |
OLC2132721432 |
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520 | |a Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. | ||
650 | 4 | |a laminar flame | |
650 | 4 | |a ethanol combustion | |
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700 | 1 | |a Lobasov, A. S. |4 aut | |
700 | 1 | |a Tolstoguzov, R. V. |4 aut | |
700 | 1 | |a Dulin, V. M. |4 aut | |
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10.1134/S001050822205001X doi (DE-627)OLC2132721432 (DE-He213)S001050822205001X-p DE-627 ger DE-627 rakwb eng 660 VZ Sharaborin, D. K. verfasserin aut Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF Lobasov, A. S. aut Tolstoguzov, R. V. aut Dulin, V. M. aut Enthalten in Combustion, explosion and shock waves Pleiades Publishing, 1966 58(2022), 5 vom: Okt., Seite 507-515 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:58 year:2022 number:5 month:10 pages:507-515 https://doi.org/10.1134/S001050822205001X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE AR 58 2022 5 10 507-515 |
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10.1134/S001050822205001X doi (DE-627)OLC2132721432 (DE-He213)S001050822205001X-p DE-627 ger DE-627 rakwb eng 660 VZ Sharaborin, D. K. verfasserin aut Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF Lobasov, A. S. aut Tolstoguzov, R. V. aut Dulin, V. M. aut Enthalten in Combustion, explosion and shock waves Pleiades Publishing, 1966 58(2022), 5 vom: Okt., Seite 507-515 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:58 year:2022 number:5 month:10 pages:507-515 https://doi.org/10.1134/S001050822205001X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE AR 58 2022 5 10 507-515 |
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10.1134/S001050822205001X doi (DE-627)OLC2132721432 (DE-He213)S001050822205001X-p DE-627 ger DE-627 rakwb eng 660 VZ Sharaborin, D. K. verfasserin aut Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF Lobasov, A. S. aut Tolstoguzov, R. V. aut Dulin, V. M. aut Enthalten in Combustion, explosion and shock waves Pleiades Publishing, 1966 58(2022), 5 vom: Okt., Seite 507-515 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:58 year:2022 number:5 month:10 pages:507-515 https://doi.org/10.1134/S001050822205001X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE AR 58 2022 5 10 507-515 |
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10.1134/S001050822205001X doi (DE-627)OLC2132721432 (DE-He213)S001050822205001X-p DE-627 ger DE-627 rakwb eng 660 VZ Sharaborin, D. K. verfasserin aut Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF Lobasov, A. S. aut Tolstoguzov, R. V. aut Dulin, V. M. aut Enthalten in Combustion, explosion and shock waves Pleiades Publishing, 1966 58(2022), 5 vom: Okt., Seite 507-515 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:58 year:2022 number:5 month:10 pages:507-515 https://doi.org/10.1134/S001050822205001X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE AR 58 2022 5 10 507-515 |
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10.1134/S001050822205001X doi (DE-627)OLC2132721432 (DE-He213)S001050822205001X-p DE-627 ger DE-627 rakwb eng 660 VZ Sharaborin, D. K. verfasserin aut Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022 Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF Lobasov, A. S. aut Tolstoguzov, R. V. aut Dulin, V. M. aut Enthalten in Combustion, explosion and shock waves Pleiades Publishing, 1966 58(2022), 5 vom: Okt., Seite 507-515 (DE-627)12959282X (DE-600)240334-1 (DE-576)015085570 0010-5082 nnns volume:58 year:2022 number:5 month:10 pages:507-515 https://doi.org/10.1134/S001050822205001X lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY SSG-OLC-CHE AR 58 2022 5 10 507-515 |
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Sharaborin, D. K. |
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Sharaborin, D. K. ddc 660 misc laminar flame misc ethanol combustion misc droplet-laden air flow combustion misc OH PLIF misc planar thermometry misc two-line OH PLIF Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF |
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660 VZ Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF laminar flame ethanol combustion droplet-laden air flow combustion OH PLIF planar thermometry two-line OH PLIF |
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temperature measurement in a bunsen gas–droplet flame of ethanol using oh plif |
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Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF |
abstract |
Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. © Pleiades Publishing, Ltd. 2022 |
abstractGer |
Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. © Pleiades Publishing, Ltd. 2022 |
abstract_unstemmed |
Abstract This paper presents the results of two-line OH planar laser-induced fluorescence (PLIF) thermometry in a laminar conical flame of a gas–droplet mixture of ethanol and air. Laminar flow of a droplet-laden ethanol–air uniform mixture was produced by an ultrasonic atomizer in a vessel filled with liquid ethanol. The properties of the two-phase flow at the nozzle exit without combustion were controlled by a time-shift optical sensor. The temperature field was estimated based on the excitation of the $$Q_{1}$$(5) and $$Q_{1}$$(14) lines of the (1–0) band of the $$A^{2}\Sigma ^{ + }$$–$$X^{2}\Pi$$electronic system. The spatial nonuniformity of the energy distribution in the laser light sheet illuminating the central plane of the flame cone and the change in the pulse energy from frame to frame were compensated using an additional camera recording the laser light intensity distribution in the calibration cuvette. © Pleiades Publishing, Ltd. 2022 |
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5 |
title_short |
Temperature Measurement in a Bunsen Gas–Droplet Flame of Ethanol Using OH PLIF |
url |
https://doi.org/10.1134/S001050822205001X |
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author2 |
Lobasov, A. S. Tolstoguzov, R. V. Dulin, V. M. |
author2Str |
Lobasov, A. S. Tolstoguzov, R. V. Dulin, V. M. |
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12959282X |
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doi_str |
10.1134/S001050822205001X |
up_date |
2024-07-03T14:40:29.979Z |
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