短舱进气道声衬优化设计与降噪机理

Optimization design and noise reduction mechanism of a nacelle inlet acoustic liner

  • 摘要: 针对某航空发动机短舱进气道声衬,开展降噪机理分析,并构建Kriging代理模型对其进行优化设计。首先,建立二维轴对称声传播数值模型,采用线性化欧拉方程(linearized Euler equations, LEE)描述声波在非均匀背景流场(入口Ma = 0.2、风扇端Ma = 0.5)中的传播;其次,结合管道声模态理论,分析不同频率下声模态的截止特性与传播规律;基于声衬阻抗边界条件求解声场分布,并对比不同周向模态和频率下的管道模态云图,分析声衬的降噪机理。结果表明,声衬能够破坏原有模态的对称性,同时激发高阶径向模态,将声能量耗散掉。最终,以传输损失(transmission loss, TL)为评价指标,采用Kriging代理模型结合遗传算法对腔深、板厚、孔径及穿孔率四个结构参数进行优化,所建立的代理模型具有较高的预测准确性(R2 = 0.94)。研究表明,基于Kriging代理模型优化所得的声衬配置(深18 mm、板厚1.01 mm、孔径1.2mm、穿孔率3.2%),在0~4000 Hz频段内的总体传输损失有所提升。模态声压云图与传输损失曲线进一步证实,该优化设计能更有效地改善声场的整体能量分布。

     

    Abstract: This study investigates the noise reduction mechanism of an aero-engine nacelle inlet acoustic liner and constructs a Kriging surrogate model for its optimization design. First, a two-dimensional axisymmetric numerical model for acoustic propagation is established, employing the linearized Euler equations to describe sound wave propagation in a non-uniform background flow field (inlet Mach number 0.2, fan-stage Mach number 0.5). Second, combined with duct acoustic mode theory, the cut-off characteristics and propagation behavior of acoustic modes at different frequencies are analyzed. The acoustic field distribution is solved using impedance boundary conditions for the liner, and the noise reduction mechanism is interpreted by comparing mode contour plots for different circumferential modes and frequencies. Results indicate that the acoustic liner disrupts the symmetry of the incident mode while exciting higher-order radial modes, thereby dissipating acoustic energy. Finally, using transmission loss as the evaluation metric, a Kriging surrogate model coupled with a genetic algorithm is used to optimize four structural parameters: cavity depth, faceplate thickness, orifice diameter, and porosity. The established surrogate model demonstrates high predictive accuracy (R2 = 0.94). Results show that the optimized liner configuration (cavity depth 18 mm, faceplate thickness 1.01 mm, orifice diameter 1.2 mm, porosity 3.2%) achieves improved overall transmission loss over the 0–4000 Hz frequency range. Modal pressure contour plots and transmission loss curves further confirm that the optimized design more effectively improves the overall energy distribution of the acoustic field.

     

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