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Additive Effects on the Burning Velocity of Ethylene-Air Mixtures

机译:对乙烯-空气混合物燃烧速度的加和效应

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Using a simple correlation based on the cubic law of early pressure rise during a closed vessel explosion, the laminar burning velocities of the stoichiometric ethylene-air mixture diluted with several additives (Ar, N_2, and CO_2) (concentrations between 4 and 40 vol %) were calculated from pressure-time records, at total initial pressures between 0.2 and 1.2 bar and ambient initial temperature. These are important input properties for numerical modeling of explosion propagation in closed or vented enclosures and for safety recommendations concerning the necessary inert gas addition. The decrease of burning velocities determined by the increase of the total initial pressure and inert gas addition is examined. A computational study of free laminar premixed flames of ethylene-air in the presence of the same additives based on the use of 53 species and an extended reaction mechanism with 592 elementary reactions delivered the temperature and species profiles in the Hame front, together with the flame width and burning velocity. Both the computed and the experimental burning velocities versus the additive concentration follow the same trend, explained by the influence of additives on the overall reaction rate between fuel and oxidant in the reaction zone and heat- and mass-transfer rates between the burned and unburned gases. The differences observed between computed and experimental burning velocities are small and can be assigned to both unavoidable scattering of available measurements and the mechanism used for numerical simulations.
机译:使用基于封闭容器爆炸期间早期压力上升的立方律的简单相关性,化学计量的乙烯-空气混合物的层流燃烧速度用几种添加剂(Ar,N_2和CO_2)稀释(浓度在4至40 vol%之间) )是根据压力时间记录在0.2至1.2 bar的总初始压力和环境初始温度下计算得出的。这些是重要的输入属性,对于在封闭或通风的外壳中爆炸传播的数值模型以及有关必需的惰性气体添加的安全建议,都是重要的输入属性。考察了由总初始压力的增加和惰性气体添加量决定的燃烧速度的降低。在使用相同的添加剂的情况下,基于乙烯和空气的自由层流预混火焰的计算研究,基于使用53种物质以及具有592个基本反应的扩展反应机理,在火焰和哈姆峰中提供了温度和物质分布宽度和燃烧速度。计算得出的燃烧速度和实验燃烧速度相对于添加剂浓度的变化趋势相同,这可以通过添加剂对反应区内燃料和氧化剂之间的总反应速率以及已燃烧和未燃烧气体之间的传热和传质速率的影响来解释。在计算的和实验的燃烧速度之间观察到的差异很小,可以归因于可用测量值的不可避免散射和用于数值模拟的机制。

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