汽车周围压力场的波数-频谱分析

Xifeng Wang, Kenta Mizushiri, H. Yokoyama, A. Iida
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引用次数: 1

摘要

为了评价汽车周围流动引起的车内噪声,有必要弄清车身表面压力波动的性质。流体运动引起的飞行器周围压力波动可以用非定常可压缩Navier-Stokes方程求解。但是,流场的动水压力波动(HPF)与气动声(声压波动APF)相关的压力波动的尺度和强度差异较大,可以作为两种不同的现象单独考虑。这一假设可以帮助我们理解压力波动这两个分量对汽车结构振动和车内声音的贡献。由于HPF和APF都是压力波动,因此不能仅通过单个压力传感器进行测量来分离它们。在本研究中,我们使用波数-频谱分析对这些压力波动进行了划分。风洞实验结果表明,高功率滤波器和有源滤波器在后视镜尾迹处具有不同的波数场,且高功率滤波器的强度和波数均大于有源滤波器。利用不可压缩流动模拟对流场进行了研究。基于车体周围压力场的波数-频谱分析表明,在车顶边界层等无分离的边界层流场中,高功率流场与有源动力流场的波数不同。另一方面,尽管进行了不可压缩模拟,但在后视镜周围下游的再循环流动中观察到HPF的波数分量非常小。这可能是由于在分离流区,流场相对于车体表面(侧护罩)向接近垂直的方向激励车体,在护罩表面上的波数矢量投影明显变小。波数矢量变短,但频率不变,导致压力传播速度明显加快。在反向流动区,即使均匀流动速度小于声速,HPF仍然可能有助于振动和声音的产生。同时,由于在反向流动区域流速实际上是减慢的,因此也观察到较大的波数分量。因此,在较宽的波长范围内可以观察到波数谱。综上所述,通过研究波数频谱,可以估计出对汽车内部噪声有贡献的流场。
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Wavenumber-Frequency Spectrum Analysis of Pressure Fields Around an Automobile
In order to evaluate the interior noise caused by the flow around automobiles, it is necessary to clarify the nature of the pressure fluctuations on the surface of vehicle body. The pressure fluctuations around the vehicle which are caused by the fluid motion can be solved by unsteady-compressible Navier-Stokes equation. However, the differences between the scales and intensity of the pressure fluctuations related to the hydrodynamic pressure fluctuation (HPF) of the flow field and the aerodynamic sound (acoustic pressure fluctuation APF) are quite large, these phenomena can be considered separately as two different phenomena. This assumption can help us to understand the contributions of these two components of pressure fluctuations to the structural vibration and interior sound of automobiles. Since both the HPF and the APF are pressure fluctuations, they cannot be separated only by measuring with a single pressure sensor. In this study, we divided these pressure fluctuations by using wavenumber-frequency spectrum analysis. Wind tunnel experiment showed that the HPF and the APF have different wavenumber fields in the wake of a rear-view mirror, and the intensity and wavenumber of the HPF are larger than that of the APF. Flow field was also investigated by using the incompressible flow simulation. As a result of wavenumber-frequency spectrum analysis based on the pressure fields around the vehicle body, the HPF and the APF have different wavenumbers in the case of a boundary layer flow field with no separation such as boundary layer on the vehicle roof. On the other hand, very small wavenumber components of the HPF were observed in the recirculation flow around the rear-view mirror downstream, despite incompressible simulation was done. This is probably due to the flow fields excite the vehicle body in the direction close to the vertical with respect to the vehicle body surface (side shield) in the separated flow region, and the wavenumber vector project on the shield surface apparently become smaller. The wavenumber vector becomes short but the frequency is constant, which leads the speed of pressure propagation apparently increases. In the reverse flow region, even if the uniform flow velocity is smaller than the speed of sound, the HPF may still contribute to vibration and sound generation. At the same time, since the flow velocity is actually slowed in the reverse flow region, large wavenumber components were also observed. Therefore, the wavenumber spectrum was observed in a wide range of the wavelength region. In conclusion, by investigating the wavenumber frequency spectrum, it is possible to estimate the flow field contributing to the interior noise of automobiles.
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