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Numerical analysis of combustion of a hydrogen-air mixture in an advanced ramjet combustor model during activation of O-2 molecules by resonant laser radiation

机译:通过谐振激光辐射激活O-2分子激活过程中氢气混合物燃烧氢气混合物燃烧的数值分析

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This paper presents a numerical study of the combustion of a hydrogen-air mixture in a model ramjet combustor with separate hydrogen and air supply during activation of O-2 molecules by resonant laser radiation at a wavelength of 762.3 nm and 193.3 nm. The calculation is made using the parabolized Navier-Stokes equations taking into account chemical reactions, laser irradiation, and the nonuniformity of air parameters at the combustor inlet due to the complex gas-dynamic structure of the flow in the air intake. It is shown that the combustion completeness at the combustor outlet can be increased by a factor of 2.8 by redistributing the hydrogen supply through the system of fuel tank pylons. Further increase in the combustion completeness can be obtained by exposure of a narrow flow region to resonant laser radiation, more effectively at a wavelength of 193.3 nm. The combination of laser exposure with hydrogen supply redistribution increases the combustion efficiency by a factor of more than 4.7 compared to the base case. In this case, this provides a 95% increase the longitudinal force component in the portion of the internal engine duct that provides a positive contribution to the thrust. Estimation of the energy efficiency of using laser radiation shows that the laser energy input required to achieve this effect is 40-80 times (depending on the fuel supply method) less than the increase in the chemical energy (compared to the case of no laser exposure) released due to fuel combustion.
机译:本文介绍了在模型Ramjet燃烧器中燃烧氢气混合物的数值研究,其在激活O-2分子的激活期间通过谐振激光辐射以762.3nm和193.3nm的激光辐射激活。通过考虑化学反应,激光照射和在燃烧器入口处的空气参数的不均匀性,由于进气中的流动的复杂气体动态结构,计算了计算的计算。结果表明,通过将氢气供应通过燃料箱塔架的系统重新分配氢供应,燃烧器出口处的燃烧完整性可以增加2.8因子。通过暴露窄流动区域以使激光辐射曝光更有效地在193.3nm的波长下,可以获得燃烧完整性的进一步增加。与基础壳体相比,激光曝光与氢气供应再分配的组合增加了燃烧效率超过4.7。在这种情况下,这提供了95%的内部发动机管道部分中的纵向力分量增加了对推力的积极贡献。使用激光辐射的能效的估计表明,实现这种效果所需的激光能量输入是40-80次(取决于燃料供应方法)小于化学能量的增加(与无激光曝光的情况相比)由于燃料燃烧而释放。

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