Inlet design and experimental verification of matching axial supersonic through-flow fan
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摘要:
针对某轴向超声速通流风扇设计与之匹配的轴对称进气道,提出了一种适用于此类进气道的设计方法,此类进气道无扩张段结构,出口即为喉道,全流场超声速。首先以
Ma 0=2.5为设计点设计初始进气道并探究了半锥角等典型参数对进气道的影响,结果表明:随半锥角增大,进气道出口总压恢复系数σ 增大、长度缩短。经分析,缩短进气道长度对于提升进气道出口σ 较为有效。将内压段中心体型面以曲面形式设计缩短进气道长度并设计试验模型进行风洞试验,此方案进气道长度缩短了约23.3%,数值模拟结果表明,在Ma 0=2.5和2.0下的不同攻角工况,进气道出口σ 提升;数值模拟的中心体沿程压力曲线和外压段纹影与风洞试验吻合较好,验证了本文数值模拟方法和进气道设计方法的正确性。Abstract:Aiming at the axisymmetric inlet designed for an axial supersonic through-flow fan, a design method suitable for this kind of inlet is proposed. This kind of inlet has no expansion section structure, the outlet is the throat, and the whole flow field is supersonic. Firstly, the initial inlet is designed with
Ma 0=2.5 as the design point, and the influence of typical parameters such as half cone angle on the inlet is explored. The results show that with the increase of half cone angle, the total pressure recovery coefficientσ at the outlet of the inlet increases and the length decreases. After analysis, shortening the inlet length is more effective for improving theσ . The central body surface of the internal pressure section is designed in the form of curved surface to shorten the length of the inlet and the test model is designed for wind tunnel test. The length of the inlet is shortened by about 23.3%. The numerical simulation results show that theσ of the inlet increases at different angles of attack atMa 0=2.5 and 2.0. The curve of pressure ratio along the center of the numerical simulation and the schlieren of the external pressure section are in good agreement with the wind tunnel test, which verifies the correctness of the numerical simulation method and the inlet design method in this paper. -
表 1 不同疏密度网格节点数
Table 1. Number of grid nodes with different density
网格疏密
程度2D 3D 节点数/
104底层网格
尺度/mm节点数/
104底层网格
尺度/mm粗糙 2.8 0.01 186 0.01 适中 7 0.0005 466 0.006 较密 11 0.0005 900 0.006 表 2 2D、3D进气道数值模拟气动参数
Table 2. Numerical simulation of inlet aerodynamic parameters of 2D and 3D
空间维度 π σ 2D 1.71 0.927 3D 1.70 0.926 表 3 两种型面控制方案进气道部分气动参数
Table 3. Partial aerodynamic parameters of inlet under two surface control schemes
方案 Mae σ ϕ A 2.07 0.928 0.998 B 2.17 0.945 0.998 表 4 Profile 2和Profile 3部分气动参数对比
Table 4. Comparison of partial aerodynamic parameters between the Profile 2 and the Profile 3
Ma0 构型 Mae σ ϕ 2.5 Profile 2 2.19 0.925 0.998 Profile 3 2.17 0.945 0.998 2.0 Profile 2 1.75 0.942 0.955 Profile 3 1.75 0.958 0.955 1.5 Profile 2 1.26 0.959 0.906 Profile 3 1.28 0.966 0.906 0.8 Profile 2 0.77 0.987 0.831 Profile 3 0.77 0.983 0.827 表 5 风洞来流参数(Ma0=0)
Table 5. Wind tunnel inflow parameters (Ma0=0)
来流静压$p_0 $/Pa 来流总压$p_0^* $/Pa 来流总温T*/K 23520 184031 297 -
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