Combustion 2008
DOI: 10.1016/b978-0-12-088573-2.00004-x
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Flame Phenomena in Premixed Combustible Gases

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Cited by 9 publications
(5 citation statements)
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“…where D = λ ρ•c P is the thermal diffusivity of the flammable mixture, C 0 is the total initial fuel concentration, T f is the end temperature in the flame front, and n and E a are the overall activation parameters (reaction order and activation energy) of the oxidation reaction [74]. The thermophysical properties of CH 4 , H 2 , O 2 , and N 2 are listed in Table 4.…”
Section: Resultsmentioning
confidence: 99%
“…where D = λ ρ•c P is the thermal diffusivity of the flammable mixture, C 0 is the total initial fuel concentration, T f is the end temperature in the flame front, and n and E a are the overall activation parameters (reaction order and activation energy) of the oxidation reaction [74]. The thermophysical properties of CH 4 , H 2 , O 2 , and N 2 are listed in Table 4.…”
Section: Resultsmentioning
confidence: 99%
“…The design and manufacture of micro burners, which have dimensions at the millimeter or submillimeter level, pose unique challenges when compared to conventional combustors, which make it not trivial to obtain a stable flame, as documented in Hossain and Nakamura [10], Ju and Maruta [1], Nakamura et al [2], Resende et al [11], and Lee et al [12]. These challenges extend to combustion in microscale environments, where the effects of viscosity are amplified in small channels, the physical residence time of mixed gases is shortened, and the ratio of area to volume of the combustion chamber increases sharply [13,14]. These factors have direct or indirect effects on the flame and the heat release of chemical energy, thereby leading to significant differences in combustion characteristics between micro and conventional combustors [15]:…”
Section: Challenges Within Microcombustionmentioning
confidence: 99%
“…A cold swirling flow of oxygen passes near the combustion chamber wall, effectively protecting it from the high temperature of the flame, which could reach up to 3030 K for the stoichiometric mixture at 1 atm, according to [14]. A gas mixture exiting the igniter is always oxidizer-rich, which helps, on the one hand, to cool down effectively the igniter wall, and on the other hand, to initiate combustion inside a solid fuel ramjet [17] or hybrid rocket engine [18] with solid fuel grain of paraffin or high-density polyethylene tested in the Laboratory.…”
Section: Ignitermentioning
confidence: 99%
“…Experimental tests provided in the Laboratory [2] entirely discovered this problem. Therefore, flow conditions favorable for ignition must be created inside the igniter, which is generally characterized by a slow flow velocity close to the flame velocity for methane-oxygen mixtures, previously discussed in [2,14,15].…”
Section: Introductionmentioning
confidence: 99%