Effect of wind velocity on flame spread in microgravity
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作者:
Prasad, K
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Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USANatl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Prasad, K
[1
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Nakamura, Y
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Nakamura, Y
Olson, SL
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Olson, SL
Fujita, O
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Fujita, O
Nishizawa, K
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Nishizawa, K
Ito, K
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Ito, K
Kashiwagi, T
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机构:Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
Kashiwagi, T
机构:
[1] Natl Inst Stand & Technol, Bldg & Fire Res Lab, Gaithersburg, MD 20899 USA
[2] Nagoya Univ, Dept Mech Engn, Nagoya, Aichi, Japan
[3] NASA, Glenn Res Ctr, Micrograv Combust Sci Branch, Cleveland, OH 44135 USA
[4] Hokkaido Univ, Dept Mech Engn, Sapporo, Hokkaido 060, Japan
A three-dimensional, time-dependent model is developed describing ignition and subsequent transition to flame spread over a thermally thin cellulosic sheet heated by external radiation in a microgravity environment. A low Mach number approximation to the Navier-Stokes equations with global reaction rate equations describing combustion in the gas phase and the condensed phase is numerically solved. The effects of a slow external wind (1-20 cm/s) on flame transition are studied in an atmosphere of 35% oxygen concentration. The ignition is initiated at the center part of the sample by generating a line-shape flame along the width of the sample. The calculated results are compared with data obtained in the 10 s drop tower. Numerical results exhibit flame quenching at a wind speed of 1.0 cm/s, two localized flames propagating upstream along the sample edges at 1.5 cm/s, a single line-shape flame front at 5.0 cm/s, and three flames structure observed at 10.0 cm/s (consisting of a single line-shape flame propagating upstream and two localized flames propagating downstream along sample edges), followed by two line-shape flames (one propagating upstream and another propagating downstream) at 20.0 cm/s. These observations qualitatively compare with experimental data. Three-dimensional visualization of the observed flame complex, fuel concentration contours, oxygen and reaction rate isosurfaces, and convective and diffusive mass flux are used to obtain a detailed understanding of the controlling mechanism. Physical arguments based on the lateral diffusive flux of oxygen, fuel depletion, the oxygen shadow of the flame, and the heat release rate are constructed to explain the various observed flame shapes.
机构:
San Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USASan Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USA
Carmignani, Luca
Bhattacharjee, Subrata
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San Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USASan Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USA
Bhattacharjee, Subrata
Olson, Sandra L.
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NASA, Glenn Res Ctr, Cleveland, OH USASan Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USA
Olson, Sandra L.
Ferkul, Paul V.
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NASA, Glenn Res Ctr, Cleveland, OH USASan Diego State Univ, Dept Mech Engn, 5500 Campanile Dr, San Diego, CA 92182 USA