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Numerical investigations on reignition behavior of detonation diffraction

机译:爆轰衍射复燃行为的数值研究

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In this paper, by adopting a fifth-order weighted essentially non-oscillatory (WENO) scheme with a third-order TVD Runge-Kutta time stepping method for two-dimensional reactive Euler equations, a parallel code is developed, and reignition behavior after a self-sustaining detonation from the tube into free space filled with H-2/O-2 mixtures is investigated. The numerical results show that the initial pressure has a great influence on the detonation cellular width, and that as the initial pressure increases, the cellular width gradually decreases and the cellular shape changes from irregular structure to regular structure, demonstrating the detonation instability to stability transition. When the initial pressure is larger than 1.2 atm, the detonation wave expands over the edge of the splitter plate, reignition can come into being because enough transverse waves collide with each other at the leading edge of the expanding front. When the initial pressure is 1.2 atm, hot spots appear on the front, and ignite the combustible gas near the hot spots after detonation diffraction. When the initial pressure is 1.0 atm, reignition fails. These findings hint that critical initial pressure exists between 1.0-1.2 atm for direct reignition after detonation diffraction.
机译:本文采用二维三阶TVD Runge-Kutta时间步长方法,采用五阶加权基本非振荡(WENO)方案和三阶TVD Runge-Kutta时间步长法,开发了并行代码,并在二次振荡后重新点燃行为研究了从管到充满H-2 / O-2混合物的自由空间的自持爆炸。数值结果表明,初始压力对爆轰胞孔宽度影响很大,随着初始压力的增大,胞孔宽度逐渐减小,胞孔形状由不规则结构转变为规则结构,证明了爆轰的不稳定性向稳定性过渡。 。当初始压力大于1.2个大气压时,爆震波会在分流板的边缘扩展,由于在扩展前缘的前缘有足够的横向波相互碰撞,因此会引起重燃。当初始压力为1.2 atm时,热点出现在前部,并在爆轰衍射后点燃热点附近的可燃气体。当初始压力为1.0 atm时,点火失败。这些发现表明,爆轰衍射后直接着火的临界初始压力在1.0-1.2atm之间。

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