Analytical model of jet shielding
Analytical model of jet shielding
复制标题
射流屏蔽解析模型
DOI:
10.2514/3.8135
复制
发表时间:
1982
期刊:
影响因子:
2.5
通讯作者:
C. Gerhold
中科院分区:
文献类型:
--
作者:
C. Gerhold
An analytical model of the shielding of a stationary point noise source by a cylindrical jet is developed. The directivity function is derived which estimates the normalized sound pressure level at a far field receiver. The shielding model is compared to experimental data for a point noise source impinging on an unheated air jet and on a simulated hot air jet. The model compares favorably to measured shielding at receiver locations away from the jet axis. The trend of the estimated shielding diverges from the measured data as the jet axis is approached. Refinement of the model is discussed. STIMATION of aircraft generated noise includes identification not only of the sources of noise on the aircraft, but also of the propagation path between the source and receiver. One of the numerous factors affecting the noise transmission path is shielding of one jet by another. The shielding jet, because of the high temperature and flow speed with respect to the immediate surroundings, acts as a partial barrier between the source and the receiver. The resultant noise reduction not only affects the overall aircraft noise level, but also indicates the possibility of jet engine in- stallation as a means of aircraft noise control. The problem of reflection and transmission of sound by a moving medium has been addressed assuming a plane wave incident on a plane surface.1"4 Ray tracing techniques have been applied to two-dimensional jets5 and cold jets.6 The two- dimensional formulation, for a cylindrical noise source impinging on the shielding jet has been developed.7 The present study is an extension to three dimensions of the previous analysis.7 The model developed consists of the sound field emitted from a stationary, discrete frequency point source, which impinges on a cylinder of locally parallel flow. The temperature and velocity profiles are uniform in the jet at any location downstream of the nozzle. While this model is an idealization of the twin jet, it is felt to incorporate the basic elements essential for a realistic representation; not only of the source, but also of the shielding jet. Model Development Formulation of the Model The mechanisms by which shielding occurs are reflection of sound at the boundary between the jet and the surrounding air and by diffraction around the jet. The noise source is modeled by a stationary discrete frequency point source located at (r0, 0,0). The shielding jet is a cylinder of radius a, and is infinite in extent along the z axis. The temperature and flow velocity are uniform across the cylinder cross section. The model is illustrated in Fig. 1. The expression for acoustic velocity potential is written for two regions; region I is outside the jet, region II is within the jet. In region I (outside the flow) In region II (inside the flow)