| 研究生: |
鄧聖儒 Teng, Sheng-Ju |
|---|---|
| 論文名稱: |
凹槽於馬赫 2 流場之燃油噴霧分布特性研究 Distribution of Liquid Fuel Spray with Cavity Flame Holder in Mach 2 Air Flow |
| 指導教授: |
袁曉峰
Yuan, Hisao-Feng |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 航空太空工程學系 Department of Aeronautics & Astronautics |
| 論文出版年: | 2023 |
| 畢業學年度: | 111 |
| 語文別: | 中文 |
| 論文頁數: | 73 |
| 中文關鍵詞: | 超音速燃燒衝壓引擎 、凹槽駐焰器 、上游燃油分布特性 |
| 外文關鍵詞: | scramjet, cavity flame holder, upstream fuel injection |
| 相關次數: | 點閱:46 下載:31 |
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在超音速燃燒衝壓引擎中,由於燃油停留在燃燒室的時間極為短暫,因此燃油的霧化混合特性是成功駐焰的因素之一。本研究利用反射式震波風洞產生 2 馬赫的自由流進行冷流實驗,探討凹槽駐焰器上游燃油噴注霧化的分布特性,以及燃油與凹槽的交互作用現象。實驗方法透過紋影法搭配高速攝影機觀察流場,定量分析燃油噴霧的消散長度、穿透高度以及抬升高度。本研究主要設計參數為燃油噴注孔徑(d=0.5mm、0.7mm)以及燃油側向噴注前傾角度0°及45°,改變燃油噴注與空氣自由流之動量通量比(J=3.93~7.43)進行觀察。實驗結果顯示,垂直噴注且孔徑 d=0.5mm 條件下,與平板流側向噴注相較,加入本實驗所採用的凹槽構型後,燃油噴霧具有較大的甩盪幅度,並且提升與空氣的混合效果,對於液態燃油的霧化混合具有正面的幫助。在相同動量通量比條件下,加大燃油噴注孔直徑至 d=0.7mm,因燃油液柱較粗,使燃油中心無法迅速與外部氣流接觸,會產生較長的消散長度以及較大的穿透高度。在相同動量通量比條件下,將燃油噴注角度向上游傾斜45°後,因燃油噴霧更劇烈的甩盪,使噴霧具有較短的消散長度、較大的穿透高度;同時在傾斜噴注條件下,燃油噴霧擁有較小的垂直動量分量,因此有較小的抬升高度,亦增加燃油噴霧與凹槽交互作用的程度。綜合以上消散長度、穿透高度以及抬升高度比較,顯示前傾45°的噴注模式較適合做為凹槽上游燃油噴注孔的設計。
In supersonic combustion ramjet engines, due to the extremely short residence time of fuel within the combustion chamber, the atomization and mixing characteristics of the fuel play a vital role in achieving successful flame stabilization. This study employed a reflected shock wave wind tunnel to generate a Mach 2 free stream for conducting cold flow experiments. The research aimed to investigate the distribution characteristics of atomized fuel injected upstream of a cavity flame holder and the interactive phenomena between the fuel and the cavity structure. The experimental approach involved schlieren visualization coupled with high-speed cameras to observe the flow field and quantitatively analyze parameters such as dissipation length, penetration height, and lift-off height of the fuel spray.
The primary design parameters of this study included the fuel injection hole diameter (d = 0.5mm, 0.7mm) and the fuel injection angle (0° and 45° inclination) with respect to the air stream. The variations in fuel injection momentum flux ratio (J = 3.93~7.43) were also examined. The experimental results showed that under vertical injection with a hole diameter of d = 0.5mm and the introduction of the cavity geometry (as used in the experiment), the fuel spray exhibited larger oscillation amplitudes and enhanced mixing with the air, leading to favorable atomization and mixing of the liquid fuel. Under the same conditions of momentum flux ratio, increasing the fuel injection hole diameter to d = 0.7mm resulted in a coarser fuel column, which hindered quick contact between the central fuel and the external airflow, thus leading to longer dissipation lengths and greater penetration heights.Under the conditions of the same momentum flux ratio, when the fuel injection angle was inclined 45° upstream, the more intense spray oscillation led to shorter dissipation lengths and larger penetration heights. Additionally, the inclined injection configuration resulted in a smaller vertical momentum component of the fuel spray, leading to a smaller lift-off height and a higher level of interaction between the fuel spray and the cavity structure.
Considering the comparisons of dissipation length, penetration height, and lift-off height, the inclined 45° injection mode was found to be more suitable for designing fuel injection orifices upstream of the cavity flame holder.
[1] Tian, Y., Yang, S., le, J., Zhong, F., and Tian, X.: ‘Investigation of the effects of fuel injector locations on ignition and flame stabilization in a kerosene fueled scramjet combustor’, Aerospace Science and Technology, 2017, 70
[2] Lin, K.-C., Ryan, M., Carter, C., Gruber, M., and Raffoul, C.: ‘Scalability of ethylene gaseous jets for fueling high-speed air-breathing combustors’, in Editor (Ed.)^(Eds.): ‘Book Scalability of ethylene gaseous jets for fueling high-speed air-breathing combustors’ (2009, edn.), pp. 1423
[3] Lewis, M.J.: ‘Significance of fuel selection for hypersonic vehicle range’, Journal of Propulsion and Power, 2001, 17, (6), pp. 1214-1221
[4] Huang, H., Spadaccini, L., and Sobel, D.: ‘Endothermic heat-sink of jet fuels for scramjet cooling’, in Editor (Ed.)^(Eds.): ‘Book Endothermic heat-sink of jet fuels for scramjet cooling’ (2002, edn.), pp. 3871
[5] Hsu, K.-Y., Carter, C., Gruber, M., and Tam, C.-J.: ‘Mixing study of strut injectors in supersonic flows’, in Editor (Ed.)^(Eds.): ‘Book Mixing study of strut injectors in supersonic flows’ (2009, edn.), pp. 5226
[6] Ben-Yakar, A., and Hanson, R.K.: ‘Cavity flame-holders for ignition and flame stabilization in scramjets: an overview’, Journal of propulsion and power, 2001, 17, (4), pp. 869-877
[7] Gruber, M., Baurle, R., Mathur, T., and Hsu, K.-Y.: ‘Fundamental studies of cavity-based flameholder concepts for supersonic combustors’, Journal of Propulsion and power, 2001, 17, (1), pp. 146-153
[8] Liu, Z., Ning, F., Zhai, Q., Ding, H., and Wei, J.: ‘Study on the flow characteristics in the supersonic morphing cavities using direct numerical simulation and proper orthogonal decomposition’, Wave Motion, 2021, 104, pp. 102751
[9] Malhotra, A., and Vaidyanathan, A.: ‘Aft wall offset effects on open cavities in confined supersonic flow’, Experimental Thermal and Fluid Science, 2016, 74, pp. 411-428
[10] Maurya, P.K., Rajeev, C., RR, V.K., and Vaidyanathan, A.: ‘Effect of aft wall offset and ramp on pressure oscillation from confined supersonic flow over cavity’, Experimental Thermal and Fluid Science, 2015, 68, pp. 559-573
[11] Trudgian, M.A., Landsberg, W.O., and Veeraragavan, A.: ‘Experimental investigation of inclining the upstream wall of a scramjet cavity’, Aerospace Science and Technology, 2020, 99, pp. 105767
[12] Kim, K.M., Baek, S.W., and Han, C.Y.: ‘Numerical study on supersonic combustion with cavity-based fuel injection’, International Journal of Heat and Mass Transfer, 2004, 47, (2), pp. 271-286
[13] Li, P., Wang, Z., Sun, M., and Wang, H.: ‘Numerical simulation of the gas-liquid interaction of a liquid jet in supersonic crossflow’, Acta Astronautica, 2017, 134, pp. 333-344
[14] Wu, P.-K., Kirkendall, K.A., Fuller, R.P., and Nejad, A.S.: ‘Breakup processes of liquid jets in subsonic crossflows’, Journal of Propulsion and power, 1997, 13, (1), pp. 64-73
[15] 林宇震, 李林, 张弛, and 徐华胜: ‘液体射流喷入横向气流混合特性研究进展’, 航空学报, 2014, 35, (1), pp. 46-57
[16] Fric, T., and Roshko, A.: ‘Vortical structure in the wake of a transverse jet’, Journal of Fluid Mechanics, 1994, 279, pp. 1-47
[17] Liu, Q., Baccarella, D., and Lee, T.: ‘Review of combustion stabilization for hypersonic airbreathing propulsion’, Progress in Aerospace Sciences, 2020, 119, pp. 100636
[18] Wang, Z.-g., Wu, L., Li, Q., and Li, C.: ‘Experimental investigation on structures and velocity of liquid jets in a supersonic crossflow’, Applied Physics Letters, 2014, 105, (13)
[19] Ali, M.M., and Kurian, J.: ‘Cavity-based injections into supersonic flow’, Journal of Propulsion and Power, 2005, 21, (6), pp. 1130-1132
[20] Rasmussen, C.C., Driscoll, J.F., Hsu, K.-Y., Donbar, J.M., Gruber, M.R., and Carter, C.D.: ‘Stability limits of cavity-stabilized flames in supersonic flow’, Proceedings of the Combustion Institute, 2005, 30, (2), pp. 2825-2833
[21] 林宥騰: ‘凹槽駐焰器於超音速燃燒流場之設計與分析’, 2022
[22] Jeong, E., O’Byrne, S., Jeung, I.-S., and Houwing, A.: ‘Investigation of supersonic combustion with angled injection in a cavity-based combustor’, Journal of Propulsion and Power, 2008, 24, (6), pp. 1258-1268
[23] 蘇佑翔: ‘燃料噴霧在馬赫 2 超音速氣流中的混合現象’, 2016
[24] Lee, S.-H.: ‘Characteristics of dual transverse injection in scramjet combustor, Part 1: Mixing’, Journal of Propulsion and Power, 2006, 22, (5), pp. 1012-1019
[25] Lin, K.-C., Kennedy, P., and Jackson, T.: ‘Structures of water jets in a Mach 1.94 supersonic crossflow’, in Editor (Ed.)^(Eds.): ‘Book Structures of water jets in a Mach 1.94 supersonic crossflow’ (2004, edn.), pp. 971
[26] 沈煒智: ‘支架於超音速流場之燃油噴注現象與混合特性探討’, 2021
[27] 楊凱文: ‘超音速流場液態燃料噴注之凹槽駐焰特性觀察’, 2022
[28] 沈雅蓁: ‘側向雙垂直噴注於超音速空氣流場之霧化混合探討’, 2015
[29] 朱國勝: ‘側向噴注於超音速流場之不穩定特性初步分析’, 2018