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Influence of After-burning Chamber Dome Length on Secondary Combustion for Solid Ducted Rocket Motor

机译:后燃室圆顶长度对固体管道火箭发动机二次燃烧的影响

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This paper is aimed at the secondary combustion in Solid Ducted Rocket (SDR) after-burning chamber, according to the analysis of ignition and combustion of boron particle and the calculating results of fuel-rich propellant. The 3D reaction flow field in the after-burning chamber of solid ducted rocket motor with binary dual-underside inlet mode was numerically simulated by means of k-ε turbulence model and one step eddy-dissipation combustion model change trend of combustion efficiency in afterburning chamber was obtained. The after-burning chamber dome lengths are set at about 45mm and 120mm, and the length of the after-burning is 400mm. The influence of after-burning chamber dome length on secondary combustion efficiency and flow field were analyzed with compared the numerical results and the experimental results. The results show that, enough length of afterburning chamber is necessary for the secondary combustion. Increasing of the dome length can the average detention time of boron particles in the head of after-burning chamber significantly, and the ignition of the boron particles can be enhanced. The boron particles resorting time is about 0.3ms in the afterburning chamber dome length is 45mm, and the boron particles resorting time is about 0.55ms in afterburning chamber dome length is 120mm. Therefore, the combustion efficiency of the boron particles in the 120mm chamber dome length is 66.4%, which higher than the one in the 45mm chamber dome length is 64.6%. And the results also show that, the dome length of after-burning chamber has little influence on the combustion efficiency in the same length of the after-burning chamber. The combustion efficiencies are 91.3% and 91.9% when the chamber dome length is set at about 45mm and 120mm correspondingly. The results of the numerical simulation are consistent well with the ground experiments results.
机译:通过对硼粒子的点火燃烧,富燃料推进剂的计算结果的分析,针对固体管道火箭后燃室的二次燃烧。利用k-ε湍流模型和后燃烧室燃烧效率的一步消散燃烧模型变化趋势,对二元双底进气模式固体管火箭发动机后燃烧室中的3D反应流场进行了数值模拟。获得了。后燃室圆顶的长度设定为约45mm和120mm,后燃室的长度为400mm。比较了数值结果和实验结果,分析了后燃室穹顶长度对二次燃烧效率和流场的影响。结果表明,二次燃烧需要足够长的后燃室。圆顶长度的增加可以显着地延长后燃烧室头部中硼颗粒的平均滞留时间,并且可以增强硼颗粒的着火性。在后燃室圆顶长度为45mm的情况下,硼粒子的恢复时间约为0.3ms,在后燃室圆顶长度为120mm的情况下,硼粒子的恢复时间约为0.55ms。因此,在120mm室穹顶长度中硼粒子的燃烧效率为66.4%,比在45mm室穹顶长度中硼粒子的燃烧效率高64.6%。结果还表明,在相同长度的后燃室中,后燃室的圆顶长度对燃烧效率的影响很小。当室穹顶长度分别设定为约45mm和120mm时,燃烧效率为91.3%和91.9%。数值模拟结果与地面实验结果吻合良好。

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