Mechanism of “heat-acoustic-vortex” coupling for transverse unstable combustion in an O2/CH4 rectangle rocket combustor
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摘要:
为了研究横向燃烧不稳定的潜在耦合机制,针对气氧/甲烷矩形火箭发动机开展了试验和数值模拟。试验采用高频压力传感器捕捉燃烧室内的动态压力特性,数值模拟采用应力混合涡模拟(SBES)和小火焰生成流(FGM)模型。结果表明:数值模拟可以准确捕捉到试验中的横向燃烧不稳定,数值计算结果在压力波形、主振频率和方均根幅值等方面与试验数据和理论结果吻合较好。对横向燃烧不稳定的驱动机理和瑞利指数进行了分析。燃烧室内流场特性表明,横向压力波会使氧气射流被周期性地“剥落”以及涡破碎,涡内燃料燃烧产生释热脉冲并耦合到燃烧室第一横向(1W)模态。瑞利因子分析表明,边缘喷嘴较中心喷嘴对横向燃烧不稳定具有更强的驱动特性。
Abstract:The potential coupling mechanism of transverse combustion instability in an O2/CH4 rectangle rocket combustor was investigated experimentally and numerically. High-frequency pressure sensors were employed to capture the dynamic pressure characteristics within the combustion chamber. Numerical simulations were conducted using the stress-blended eddy simulation (SBES) and flamelet-generated manifolds (FGM) methods. The results showed that the numerical simulation successfully predicted the transverse combustion instability observed experimentally. The numerical results, including pressure waveform, main frequency, and root mean square amplitude, were in good agreement with the experimental data and theoretical analysis. A comprehensive analysis of the driving mechanism and Rayleigh index of the transverse combustion instability was presented. Examination of the flow field characteristics in the combustion chamber revealed that the transverse pressure wave induced periodic ‘stripping’ of the oxygen jet and vortex disruption. Heat release pulses were generated during vortex fuel combustion and coupled with the first width (1W) mode. Rayleigh index analysis indicated that edge injectors exhibited stronger driving characteristics for transverse combustion instability compared with central injectors.
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表 1 热试车工况及试验结果
Table 1. Operating conditions and experimental results of hot-fire tests
参数 试验编号 1 2 3 $ p{ (\mathrm{O}}_{2}) $/MPa 2.06 2.08 2.05 $ \dot{m}{ (\mathrm{O}}_{2}) $/(g/s) 170 172 169 $ p{ (\mathrm{C}\mathrm{H}}_{4}) $/MPa 1.15 1.16 1.15 $ \dot{m}{ (\mathrm{C}\mathrm{H}}_{4}) $/(g/s) 100 101 100 pc/MPa 1.06 1.05 1.05 f/Hz 3033 3035 3029 $p'_{{\mathrm{RMS}}} $/MPa 0.195 0.196 0.188 -
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