Influence of backflow duct on the buzz of two-dimensional hypersonic inlet
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摘要:
探讨了回流通道对二维高超声速进气道喘振的影响,通过非定常数值仿真分析不同回流通道布局方案的作用机制。结果表明:在内收缩段下壁面设置回流通道,通过回流通道出口形成的弱压缩系与膨胀波系使外压缩波向外侧偏移增大溢流,进而缓解气流积蓄,抑制下游反压增长,可显著降低内收缩段区域的压强脉动,但对隔离段的高幅压强脉动的抑制效果有限;而在隔离段下壁面设置回流通道,主要是通过遏止主结尾激波前传,降低隔离段中部区域的高幅压强脉动。双回流通道布局可使整个进气道内的压强脉动显著降低,内收缩段区域和隔离段区域压强脉动方均根值降幅最高分别为43.7%和58.7%。
Abstract:The impact of backflow ducts on buzz in a two-dimensional hypersonic inlet was studied. The influence mechanisms of different backflow duct configurations were analyzed through unsteady numerical simulations. The results indicated that placing a backflow duct on the lower wall of the internal contraction section generated a weak compression system and expansion waves at the outlet, causing the external compression wave to shift outward, which increased spillage and alleviated airflow accumulation. This, in turn, suppressed downstream back-pressure growth and significantly reduced pressure fluctuations in the contraction section. However, the suppression effect on high-amplitude pressure fluctuations in the isolator section was limited. Placing a backflow duct on the lower wall of the isolator primarily curbed the forward movement of the terminal shock, reducing high-amplitude pressure fluctuations in the mid-region of the isolator. The combined layout of both backflow ducts effectively reduced pressure fluctuations throughout the entire inlet, with root mean square values in the contraction and isolator sections decreasing by up to 43.7% and 58.7%, respectively.
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图 19 完整喘振周期内γic=1.4内收缩段回流通道布局构型进气道进/出口流量系数φ及出口压强$ {{p}}_{{\mathrm{ex}}} $随时间变化曲线
Figure 19. Time variation curve of flow coefficient φ and outlet pressure $ {{p}}_{{\mathrm{ex}}} $ at inlet/outlet of γic=1.4 internal contraction section backflow duct layout configuration inlet over a complete buzz cycle
表 1 典型测点x方向坐标
Table 1. x-direction coordinate of typical measurement points
典型测点x方向坐标 x/m d1 329.088 d2 420.958 d3 480.958 d4 540.958 u1 320.958 u2 420.958 u3 480.958 u4 540.958 表 2 不同疏密度网格P7监测点处振荡频率
Table 2. Oscillation frequency at P7 monitoring point for different grid densities
数据源 主频率/Hz 疏网格 369.34 中等网格 369.12 密网格 368.35 实验数据[28] 360.00 表 3 不同疏密度网格计算的d3测点处振荡频率
Table 3. Oscillation frequency at d3 measurement point calculated with different grid densities
网格密度 主频率/Hz 疏网格 262.98 中等网格 260.52 密网格 260.92 表 4 不同时间步d3测点处振荡频率
Table 4. Oscillation frequency at d3 measurement point with different time steps
时间步长 主频率/Hz 10−4 243.77 10−5 260.52 10−6 256.62 表 5 γic=1.4基准构型进气道的喘振频率和各典型测点的 压强脉动RMS值
Table 5. Buzz frequency and pressure fluctuation RMS values at various typical measurement points of γic=1.4 baseline configuration inlet
参数 数值 f/Hz 260.41 σrms/Pa d1 22.7p0 d2 68.0p0 d3 100.6p0 d4 130.1p0 u1 29.4p0 u2 73.1p0 u3 102.4p0 u4 128.0p0 表 6 内收缩段回流通道布局构型典型测点压强脉动RMS值及其RMS值降幅
Table 6. Pressure fluctuation RMS values and RMS reduction at typical measurement points of internal contraction section backflow duct layout configuration
典型测点 压强脉动RMS值 压强脉动RMS值降幅/% u1 22.4p0 23.90 d1 17.9p0 21.12 u2 56.5p0 22.72 d2 56.0p0 17.63 u3 88.5p0 13.59 d3 89.2p0 11.37 u4 119.6p0 6.53 d4 118.6p0 8.85 表 7 隔离段回流通道布局构型典型测点压强脉动RMS值 及其RMS值降幅
Table 7. Pressure fluctuation RMS values and RMS reduction at typical measurement points of isolator section backflow duct layout configuration
典型测点 压强脉动RMS值 压强脉动RMS值降幅/% u1 29.1$ {{p}}_{0} $ 1.01 d1 22.9$ {{p}}_{0} $ −0.75 u2 77.5$ {{p}}_{0} $ −6.04 d2 69.5$ {{p}}_{0} $ −2.13 u3 55.0$ {{p}}_{0} $ 46.30 d3 58.5$ {{p}}_{0} $ 41.83 u4 130.3$ {{p}}_{0} $ −1.84 d4 127.1$ {{p}}_{0} $ 2.30 表 8 双回流通道布局构型典型测点压强脉动RMS值 及其RMS值降幅
Table 8. Pressure fluctuation RMS values and RMS reduction at typical measurement points of dual backflow duct layout configuration
典型测点 压强脉动RMS值 压强脉动RMS值降幅/% u1 16.5$ {{p}}_{0} $ 43.74 d1 13.2$ {{p}}_{0} $ 41.91 u2 55.3$ {{p}}_{0} $ 24.37 d2 51.5$ {{p}}_{0} $ 24.21 u3 42.28$ {{p}}_{0} $ 58.72 d3 48.46$ {{p}}_{0} $ 51.84 u4 116.2$ {{p}}_{0} $ 9.21 d4 110.6$ {{p}}_{0} $ 14.98 -
[1] BOWCUTT K G. Multidisciplinary optimization of airbreathing hypersonic vehicles[J]. Journal of Propulsion and Power, 2001, 17(6): 1184-1190. doi: 10.2514/2.5893 [2] KURTH G, BAUER C. Air intake development for supersonic missiles [R]. AIAA-2008-5263, 2008. [3] CHEN Hao, TAN Huijun, ZHANG Qifan, et al. Buzz flows in an external-compression inlet with partially isentropic compression[J]. AIAA Journal, 2017, 55(12): 4286-4295. doi: 10.2514/1.J056066 [4] CHEN Hao, TAN Huijun, ZHANG Qifan, et al. Throttling process and buzz mechanism of a supersonic inlet at overspeed mode[J]. AIAA Journal, 2018, 56(5): 1953-1964. doi: 10.2514/1.J056674 [5] VAN WIE D, KWOK F, WALSH R. Starting characteristics of supersonic inlets[R]. AIAA-1996-2914, 1996. [6] OSWATITSCH K. Pressure recovery for missiles with reaction propulsion at high supersonic speeds (the efficiency of shock diffusers)[EB/OL]. [2023-11-23].https://doi.org/10.1007/978-3-322-91082-0_18. [7] 张红英, 孙姝, 程克明, 等. 进气道工作状态对吸气式高超声速飞行器气动力特性影响的实验研究[J]. 宇航学报, 2007, 28(6): 1488-1493. ZHANG Hongying, SUN Shu, CHENG Keming, et al. Experimental investigation of inlet start/unstart influences on the aerodynamic characteristic of a hypersonic vehicle[J]. Journal of Astronautics, 2007, 28(6): 1488-1493. (in Chinese doi: 10.3321/j.issn:1000-1328.2007.06.010ZHANG Hongying, SUN Shu, CHENG Keming, et al. Experimental investigation of inlet start/unstart influences on the aerodynamic characteristic of a hypersonic vehicle[J]. Journal of Astronautics, 2007, 28(6): 1488-1493. (in Chinese) doi: 10.3321/j.issn:1000-1328.2007.06.010 [8] WAGNER J, VALDIVIA A, YUCEIL K, et al. An experimental investigation of supersonic inlet unstart[R]. AIAA 2007-4352, 2007. [9] WAGNER J, YUCEIL K, VALDIVIA A, et al. PIV measurements of the unstart process in a supersonic inlet/isolator[R]. AIAA 2008-3849, 2008. [10] WAGNER J L, YUCEIL K B, VALDIVIA A, et al. Experimental investigation of unstart in an inlet/isolator model in Mach 5 flow[J]. AIAA Journal, 2009, 47(6): 1528-1542. doi: 10.2514/1.40966 [11] WAGNER J L, YUCEIL K B, CLEMENS N T. Velocimetry measurements of unstart of an inlet-isolator model in Mach 5 flow[J]. AIAA Journal, 2010, 48(9): 1875-1888. doi: 10.2514/1.J050037 [12] TAN Huijun, GUO Rongwei. Experimental study of the unstable-unstarted condition of a hypersonic inlet at Mach 6[J]. Journal of Propulsion and Power, 2007, 23(4): 783-788. doi: 10.2514/1.28039 [13] TAN Huijun, SUN Shu, YIN Zhilong. Oscillatory flows of rectangular hypersonic inlet unstart caused by downstream mass-flow choking[J]. Journal of Propulsion and Power, 2009, 25(1): 138-147. doi: 10.2514/1.37914 [14] LI Zhufei, GAO Wenzhi, JIANG Hongliang, et al. Unsteady behaviors of a hypersonic inlet caused by throttling in shock tunnel[J]. AIAA Journal, 2013, 51(10): 2485-2492. doi: 10.2514/1.J052384 [15] 张启帆. 二维/三维压缩高超声速进气道不起动机理及控制研究[D]. 南京: 南京航空航天大学, 2017. ZHANG Qifan. Study on starting mechanism and control of 2D/3D compression hypersonic inlet[D]. Nanjing: Nanjing University of Aeronautics and Astronautics, 2017. (in ChineseZHANG Qifan. Study on starting mechanism and control of 2D/3D compression hypersonic inlet[D]. Nanjing: Nanjing University of Aeronautics and Astronautics, 2017. (in Chinese) [16] CHANG Juntao, WANG Lei, BAO Wen, et al. Novel oscillatory patterns of hypersonic inlet buzz[J]. Journal of Propulsion and Power, 2012, 28(6): 1214-1221. doi: 10.2514/1.B34553 [17] ZHANG Q F, TAN H J, SUN S, et al. Unstart of a hypersonic inlet with side compression caused by downstream choking[J]. AIAA Journal, 2016, 54(1): 28-38. doi: 10.2514/1.J054095 [18] SARAVANAN R, DESIKAN S L N, FRANCISE K J, et al. Experimental investigation of start/unstart process during hypersonic intake at Mach 6 and its control[J]. Aerospace Science and Technology, 2021, 113: 106688. doi: 10.1016/j.ast.2021.106688 [19] 潘瑾, 张堃元. 可变内收缩比侧压式进气道自起动性能[J]. 推进技术, 2007, 28(3): 278-281, 321. PAN Jin, ZHANG Kunyuan. Self-starting characteristics for sidewall-compression inlet with variable internal contraction ratio[J]. Journal of Propulsion Technology, 2007, 28(3): 278-281, 321. (in Chinese doi: 10.3321/j.issn:1001-4055.2007.03.013PAN Jin, ZHANG Kunyuan. Self-starting characteristics for sidewall-compression inlet with variable internal contraction ratio[J]. Journal of Propulsion Technology, 2007, 28(3): 278-281, 321. (in Chinese) doi: 10.3321/j.issn:1001-4055.2007.03.013 [20] KANG K, WERMER L, IM S, et al. Fast-acting boundary-layer suction to control unstarting and unstarted flows[J]. AIAA Journal, 2020, 58(6): 2475-2485. doi: 10.2514/1.J058887 [21] HUANG Hexia, TAN Huijun, SUN Shu, et al. A fluidic control method of shock train in hypersonic inlet/isolator[R]. AIAA 2014-3846, 2014. [22] WANG Ziao, XU Kejing, CHANG Juntao. Distributed fluidic control method for alleviating rapid movement of shock train[J]. AIAA Journal, 2022, 60(11): 6252-6269. doi: 10.2514/1.J062020 [23] VALDIVIA A, YUCEIL K B, WAGNER J L, et al. Control of supersonic inlet-isolator unstart using active and passive vortex generators[J]. AIAA Journal, 2014, 52(6): 1207-1218. doi: 10.2514/1.J052214 [24] SRIKANT S, WAGNER J L, VALDIVIA A, et al. Unstart detection in a simplified-geometry hypersonic inlet-isolator flow[J]. Journal of Propulsion and Power, 2010, 26(5): 1059-1071. doi: 10.2514/1.46937 [25] TAN Huijun, LI Liugang, WEN Yufen, et al. Experimental investigation of the unstart process of a generic hypersonic inlet[J]. AIAA Journal, 2011, 49(2): 279-288. doi: 10.2514/1.J050200 [26] WHITE F M . Viscous fluid flow[M]. New York: McGraw-Hill, 1991. [27] SPALART P, ALLMARAS S. A one-equation turbulence model for aerodynamic flows[R]. AIAA 1992-439, 1992. [28] NAGASHIMA T, OBOKATA T, ASANUMA T. Experiment of supersonic air intake buzz[J]. ISAS Report, 1972, 37(7): 165-209. [29] WANG Jianyong, XIE Lyurong, ZHAO Hao, et al. Fluidic control method for improving the self-starting ability of hypersonic inlets[J]. Journal of Propulsion and Power, 2016, 32(1): 153-160. doi: 10.2514/1.B35749 [30] YAN Li, WU Han, HUANG Wei, et al. Shock wave/turbulence boundary layer interaction control with the secondary recirculation jet in a supersonic flow[J]. Acta Astronautica, 2020, 173: 131-138. doi: 10.1016/j.actaastro.2020.04.003 -

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