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Theory of Flame Acceleration in Tubes due to Wall Friction: Intrinsic Limitations and Accuracy

机译:墙体摩擦引起的管中火焰加速度的理论:内在限制和准确性

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A slow, subsonic flame can accelerate spontaneously, with the velocity jump by several orders of magnitude and even subsequent detonation triggering. This effect is extremely crucial, in particular, for fire safety issues in mines, subways and power plants. Flame acceleration is especially strong while propagating in tubes or channels. According to the celebrative Shelkin model, the key element of the process is wall friction at non-slip walls. Indeed, as a flame front propagates from a closed tube/channel end to the open one, the burning matter expands and it drives a flow of the fresh fuel mixture. However, due to the friction on the tube walls, the flow becomes non-uniform such that the burning matter bends the flame front, increases the flame velocity and leads to the flame acceleration. During the recent years, the effect has been clarified and investigated - analytically, computationally and experimentally. In particular, the analysis of Bychkov et al. describes the entire scenario of the flame acceleration and detonation triggering, namely: (i) initial exponential acceleration in the quasi-incompressible state; (ii) moderation of the process because of gas compression, so the exponential acceleration state goes over to a slower one; (iii) eventual saturation to a steady, quasi-steady or statistically-steady, high-speed flames correlated with the Chapman-Jouguet deflagration; at the latter stage, heating of the fuel mixture leads to an explosion ahead of the flame front, which develops into a self-sustained detonation. While this analytical theory is validated by extensive direct numerical simulations of the combustion equations including transport process, chemical reactions, viscosity, thermal conduction and diffusion, it nevertheless includes a set of assumptions such as the large Reynolds number related to flame propagation, Re1, as well as the large thermal expansion coefficient in the burning process, Θ1. This therefore leads to the intrinsic limitations of the theory. In this work we determine these limitations and thereby clearly underline the validity domains in the relevant Re-Θ diagram. The present analysis also demonstrates that the theory of flame acceleration is consistence with a model of steady flame propagation developed recently.
机译:缓慢,子源火焰可以自发加速,随着速度跳跃几个数量级甚至随后的爆轰触发。这种效果尤其至关重要,特别是用于矿山,地铁和发电厂的消防安全问题。火焰加速度在管或通道中繁殖时特别强大。根据庆祝涡旋模型,该过程的关键要素是防滑墙壁的壁摩擦。实际上,由于火焰前沿从闭管/通道端传播到开放式,燃烧物膨胀,并且它驱动新鲜燃料混合物的流动。然而,由于管壁上的摩擦,流动变得不均匀,使得燃烧物弯曲火焰前部,增加火焰速度并导致火焰加速度。在近年来,在计算,计算地和实验中,效果已被澄清和调查。特别是,对Bychkov等人的分析。描述了火焰加速度和爆炸触发的整个场景,即:(i)准不可压缩状态下的初始指数加速度; (ii)由于气体压缩而促进过程,因此指数加速状态越来越慢; (iii)最终饱和度稳定,准稳态或统计稳定,高速火焰与Chapman-Jouguet净化相关;在后一阶段,燃料混合物的加热导致火焰前沿的爆炸,这导致了自我持续的爆轰。虽然该分析理论通过包括运输过程,化学反应,粘度,热传导和扩散的燃烧方程的广泛直接数值模拟验证,但是包括一组假设,例如与火焰传播相关的大型雷诺数,Re 1,以及燃烧过程中的大的热膨胀系数,θ 1。因此,这导致了理论的内在局限性。在这项工作中,我们确定这些限制,从而清楚地强调了相关的RE-θ图中的有效域。本分析还证明了火焰加速理论与最近开发的稳定火焰繁殖的模型一致。

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