Study of Acetone-OH Simultaneous PLIF for Combustion Diagnostics of Turbulent Premixed Flames

This paper described an availability of acetone-OH simultaneous PLIF scheme for combustion diagnostics on turbulent premixed flame. Distinctive signal gap is found between acetone (seeded in the premixed gas) and OH (combustion product) with single excitation wavelength and single CCD camera to achi...

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Published inNihon Kikai Gakkai rombunshuu. B hen Vol. 73; no. 725; pp. 350 - 356
Main Authors MANOME, Satoshi, YAMASHITA, Hiroshi, HAYASHI, Naoki, YAMAMOTO, Kazuhiro, NAKAMURA, Yuji
Format Journal Article
LanguageJapanese
Published The Japan Society of Mechanical Engineers 2007
Subjects
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ISSN0387-5016
1884-8346
DOI10.1299/kikaib.73.350

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Abstract This paper described an availability of acetone-OH simultaneous PLIF scheme for combustion diagnostics on turbulent premixed flame. Distinctive signal gap is found between acetone (seeded in the premixed gas) and OH (combustion product) with single excitation wavelength and single CCD camera to achieve relatively low cost measurement of flame zone. Flame zone thickness includes much flame information e.g. the location of heat release region, local burning velocity. Considered turbulent condition throughout the present study is relatively weak and categorized in laminar flamelet regime. As the equivalence ratio of premixed mixture (acetone seeded methane-air premixed gas) is varied from 0.64 to 0.90 (burning velocity is increased), measured local flame zone thickness (mode value) is decreased, however 3-D movement of the observed flame front makes the measured flame zone thickness wider than the laminar flame condition. In addition, results show that flame front curvature (convex toward unburned is positive) is positively correlated with flame zone thickness. It is ensured an applicability of the present scheme to survey the relation between flame zone thickness and flame front curvature in turbulent premixed flame.
AbstractList This paper described an availability of acetone-OH simultaneous PLIF scheme for combustion diagnostics on turbulent premixed flame. Distinctive signal gap is found between acetone (seeded in the premixed gas) and OH (combustion product) with single excitation wavelength and single CCD camera to achieve relatively low cost measurement of flame zone. Flame zone thickness includes much flame information e.g. the location of heat release region, local burning velocity. Considered turbulent condition throughout the present study is relatively weak and categorized in laminar flamelet regime. As the equivalence ratio of premixed mixture (acetone seeded methane-air premixed gas) is varied from 0.64 to 0.90 (burning velocity is increased), measured local flame zone thickness (mode value) is decreased, however 3-D movement of the observed flame front makes the measured flame zone thickness wider than the laminar flame condition. In addition, results show that flame front curvature (convex toward unburned is positive) is positively correlated with flame zone thickness. It is ensured an applicability of the present scheme to survey the relation between flame zone thickness and flame front curvature in turbulent premixed flame.
Author NAKAMURA, Yuji
MANOME, Satoshi
HAYASHI, Naoki
YAMASHITA, Hiroshi
YAMAMOTO, Kazuhiro
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References_xml – reference: (3) Giezendanner, R., Keck, O., Weigand, P., Meier, W., Meier, U., Stricker, W. and Aigner, M., Combust. Sci. and Tech., 175, (2003), pp. 721-741.
– reference: (1) Allen, M. G., Howe, R. D. and Hanson, R. K., Opt. Lett., Vol. 11, No. 3 (1986), pp. 126-128.
– reference: (12) Lozano, B., Yip, B. and Hanson, R. K., Exp. Fluids 13, (1992), pp. 369-376.
– reference: (9) Peters, N., J. Fluid Mech. 384, (1999), pp. 107-132.
– reference: (18) Sun, C. J., Sung, C. J., He, L. and Law, C. K., Combust. Flame 118, (1995), pp. 108-128.
– reference: (21) Goey, L. P. H. d., Plessing, T., Hermanns, R. T. E., Peters, N., Proc. Combust. Inst. 30, (2005), pp. 859-866.
– reference: (16) Williams, F. A., Combustion Theory, (1985), pp. 349-372, The Benjamin/Cummings Publishing Company, Inc.
– reference: (13) http://www.schott.com/optics_devices/
– reference: (6) Tanahashi, M., Murakami, S., Choi, G. M., Fukuchi, Y. and Miyauchi, T., Proc. Combust. Inst. 30, (2005), pp. 1665-1672.
– reference: (20) Chakraborty, N. and Cant, S., Combust. Flame 137, (1996), pp. 129-147.
– reference: (22) Yokomori, T. and Mizumoto, M., Proc. Combust. Inst. 29, (2002), pp. 1511-1517.
– reference: (2) Chen, Y. and Mansour, M. S., Appl. Phys. B 64, (1997), pp. 599-605.
– reference: (8) Williams, F. A., Combustion Theory, (1985), pp. 411-440, The Benjamin/Cummings Publishing Company, Inc
– reference: (19) Echekki, T. and Chen, J. H., Combust. Flame 106, (1996), pp. 184-202.
– reference: (4) Han, D. and Mungal, M. G., Combust. Flame 132, (2003), pp. 565-590.
– reference: (14) Chew, T. C., Bray, K. N. C. and Britter, R. E., Combust. Flame 80, (1990), pp. 65-82.
– reference: (7) Nakamura, Y., Manome, S., Satomi, S., Hayashi, N. and Yamashita, H., J. Combustion Society of Japan, Vol. 47, No. 142, (2005), pp. 290-299. (in Japanese)
– reference: (10) Yamamoto, N., Nakamura, Y., Zhao, D. and Yamashita, H., Fluid & Heat Eng. Res. 38, (2003), pp. 19-28. (in Japanese)
– reference: (15) Yamamoto, K., Nishizawa, Y. and Onuma, Y., JSME International J. B46-3, (2003), pp. 408-415.
– reference: (5) Watson, K. A., Lyons, K. M., Carter, C. D. and Donbar, J. M., Proc. Combust. Inst. 29, (2002), pp. 1905-1912.
– reference: (17) Lee, J. G., Lee, T. W., Nye, D. A. and Santavicca, D. A., Combust. Flame 100, (1995), pp. 161-168.
– reference: (11) Hikita, T. and Akita, K., Nensyo-Gairon, (1971), pp. 190-199, Corona-Sya. (in Japanese)
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Snippet This paper described an availability of acetone-OH simultaneous PLIF scheme for combustion diagnostics on turbulent premixed flame. Distinctive signal gap is...
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StartPage 350
SubjectTerms Acetone
Flame Front Curvature
Flame Zone Thickness
Laser
OH
Premixed Combustion
Turbelent Flow
Title Study of Acetone-OH Simultaneous PLIF for Combustion Diagnostics of Turbulent Premixed Flames
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