Air tab location effect on supersonic jet mixing

Mahendra Perumal Govindan, Aravindh Kumar Suseela Moorthi, S. Elangovan, Munisamy Sundararaj, E. Rathakrishnan
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Abstract

Mixing of Mach 2.1 circular, jet issuing from a straight convergent-divergent circular nozzle, in the presence of sonic air tabs at exit and shifted locations along the jet axis was investigated experimentally at nozzle pressure ratios (NPR) 3–6, insteps of 1. Two constant area tubes of 1 mm diameter positioned diametrically opposite, at 0 D, 0.25 D, 0.5 D and 0.75 D (where D is the nozzle exit diameter), were used for fluidic injection. The injection pressure ratio (IPR) of air tabs was maintained at 6. The Mach 2.1 jet operated at nozzle pressure ratio (NPR) in the range of overexpanded states corresponding to NPR 3–6 was controlled with the sonic air tabs operating at the underexpanded state corresponding to IPR 6. The impact of air tabs on jet mixing was studied from the measured Pitot pressure along the jet centerline. The centerline pressure decay of the jet confirms that the air tab promotes jet mixing with the entrained air mass, and the mixing promotion caused by the air tab is dependent on tab location as well as the NPR. In the presence of air tabs, the jet possesses shorter core and experiences faster decay than the uncontrolled jet. Also, the air tabs were effective in reducing the number of shock cells and rendering the waves weaker in the jet core. Among the tab locations, the mixing promoting effectiveness of air tabs at 0 D is better than the tabs at shifted locations. The jet core length reduction caused by the air tab at 0 D increases from 25.4 % to 77.2 %, with increasing NPR from 3 to 6. The same trend was noticed for tab location 0.75 D, but not for 0.25 D and 0.5 D locations. The core length reduction for 0.75 D tab location is about 61.4 %, at NPR 6, and 62.1 % and 55.8 %, for NPR 5 and 4 for tab locations 0.25 D and 0.5 D, respectively. Shadowgraph images of the waves present in the jet core confirms the findings of centerline pressure decay results.
气片位置对超音速喷流混合的影响
在喷嘴压力比(NPR)3-6、步长为 1 的条件下,实验研究了在喷嘴出口和沿喷射轴线移动位置的声波空气片存在的情况下,从直的会聚-发散圆形喷嘴喷出的马赫数为 2.1 的圆形喷流的混合情况。空气片的喷射压力比 (IPR) 保持在 6。马赫数为 2.1 的射流在喷嘴压力比 (NPR) 对应 NPR 3-6 的过扩张状态范围内运行,声波空气片则在对应 IPR 6 的欠扩张状态下运行。 根据沿射流中心线测得的皮托管压力,研究了空气片对射流混合的影响。喷流中心线压力衰减证实,气膜促进了喷流与夹带气团的混合,而气膜对混合的促进作用取决于气膜位置和 NPR。与不受控的喷流相比,在有气片的情况下,喷流的核心更短,衰减更快。此外,气垫片还能有效减少冲击单元的数量,使射流核心的波浪更弱。在各个气片位置中,0 D 处气片的混合促进效果优于偏移位置的气片。随着 NPR 从 3 到 6 的增加,0 D 位置的空气滤片导致的喷流核心长度缩减从 25.4% 增加到 77.2%。同样的趋势也出现在 0.75 D 的气嘴位置,而 0.25 D 和 0.5 D 的气嘴位置则没有。0.75 D 凸片位置的岩心长度在净波长为 6 时减少了约 61.4%,而在净波长为 5 和 4 时,0.25 D 和 0.5 D 凸片位置的岩心长度分别减少了 62.1% 和 55.8%。喷流核心中出现的波浪阴影图证实了中心线压力衰减结果。
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