| 研究生: |
黃冠雄 Huang, Guan-Shiung |
|---|---|
| 論文名稱: |
低速平面噴流擺盪運動之實驗研究 The Experimental Study on the Flapping Motion of Low-speed Plane Jet |
| 指導教授: |
蕭飛賓
Hsiao, Fei-Bin |
| 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: | 2005 |
| 畢業學年度: | 93 |
| 語文別: | 英文 |
| 論文頁數: | 75 |
| 中文關鍵詞: | 長波激擾 、擺盪運動 、平面噴流 |
| 外文關鍵詞: | Plane jet, Flapping motion, Long-wave excitation |
| 相關次數: | 點閱:142 下載:3 |
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本論文以實驗方法進行二維(2-D)平面噴流加入長波激擾其流場特性及模態之研究,並以X型熱線測速儀及煙流(Smoke-flow)進行流場之量測及觀察。實驗條件為噴流出口流速保持在5 m/s,以噴流出口高度為特徵長度所定義之雷諾數為 。實驗中以分別裝置於噴流出口上下側之兩獨立長條木片對流場進行激擾,由兩長條木片所構成之振動機構是以電磁驅動並可藉由波形產生器產生對稱與反對稱之擾動。
實驗結果發現振動機構的作動模式對噴流的擺盪特性及渦流分布有顯著之影響,可改變噴流中不穩定波在近場的演化以及下游的渦流結構。對流場施以相較於基礎頻率(fundamental frequency)的低頻激擾,則渦流開始成長的位置會較為提前且下游的渦流結構會更為強化。若施以非對稱之激擾,噴流寬度在等勢核之後會大幅成長且噴流的擺盪運動將更顯著;反之,若施以對稱之激擾,向下游傳遞之渦流會呈現對稱分布,噴流擺盪運動則被抑制。
實驗中選擇了四種低頻頻率對流場進行激擾。在不同之激擾頻率下,由流場量測及視流(flow visualization)所得之結果加以討論,以驗證長波之低頻激擾對噴流流場之影響。
Present paper investigates the behaviors and flow properties of a 2-dimensional(2-D)plane jet with long-wave excitation by hot-wire anemometric measurements and smoke-flow visualization. The jet exit velocity is operated at 5m/sec with the Reynolds number of based on the height of the jet exit. The jet was excited by two independent strips mounted to the nozzle exit. The two strips consisting the forcing mechanism were driven by electromagnetic-force and controlled by a signal generator to introduce anti-symmetric and symmetric disturbances.
The flapping features are significantly affected by the distributions of vortices and the phase relation between the upper and lower instability modes of the jet flapping mechanism. The near-field evolutions of the instability waves, as well as the downstream vortical structures, were altered by the excitations. The roll-up location moved forward and the vortices were more organized when the strips flapped in a frequency lower than the fundamental frequency. If the excitation was anti-symmetric, the flapping was enhanced and the jet spread wider after the potential core. If symmetric, the vortices shed downstream were symmetric and the flapping motion was suppressed.
Four low band excitation frequencies were chosen in the experiment. Results of the mean flow measurement and flow visualization under each excitation frequency were discussed in this thesis in order to illustrate the effect of the long-wave excitation on the jet.
[1]Crow,S.C. and Champagne,F.H., “Orderly structure in jet
turbulence”, J. Fluid Mech., Vol.48, pp.547-591, 1970
[2]Brown,F.K., Roshko,A., ”On the density effects and large structure in turbulent mixing layers”, J. Fluid Mech., Vol.64, pp.775-816, 1974
[3]Hussain,A.K.M.F., “Coherent Structures–Reality and Myth,” Phys. Fluids, vol.26, pp.2816-2850, 1983.
[4]Winant,C.D. and Browand,F.K., “Vortex pairing-the mechanism of turbulent mixing-layer growth at moderate Reynolds number”, J. Fluid Mech., Vol.63, pp.237~255, 1974.
[5]Ho,C. M., “Local and Global Dynamics of Free Shear Layers, “Proceedings of the Symposium on Numerical and Physical Aspects of Aerodynamic Flow, pp.521-533, 1982.
[6]Ho,C.M. and Huang,L.S., “Subharmonics and Vortex Merging in Mixing Layers,” J. Fluid Mech., vol.119, pp.443-473, 1982.
[7]Thomas, F. O., “Structure of Mixing Layers and Jets,” Appl. Mech. Rev., Vol.44, No. 3, pp.119~150, 1991.
[8]Hsiao,F.B. and Huang,J.M., “Subharmonic Evolution of Coherent Structures in an Excited Plane Jet,” AIAA-88-3609, 1988.
[9]Kibens,V., “Discrete noise spectrum generated by an acoustically excited jet, “AIAA Journal, Vol.18, pp.434-441, 1980
[10]Zaman,K.B.M.Q. and Hussain,A.K.M.F., “Turbulence Suppression in Free Shear Flow by Controlled Excitation,” J. Fluid Mech., vol.103, pp.133-159, 1981.
[11]Ho,C.M. and Gutmark,E., “Preferred Modes and the Spreading Rates of Jets,” Phys, Fluids, vol.26, pp.2932-2938, 1983.
[12]Weisbrot,I. and Wygnanski,I., “On Coherent Structures In a Highly Excited Mixing Layer,”J. Fluid Mech., Vol.195, pp.137~159, 1988.
[13]Greenblatt,D. and Wygnanski,I.J., “The Control of Flow Separation by Periodic Excitation,” Progress in Aerospace Sciences, Vol.36, pp,487~545, 2000.
[14]Goldschmidt,V.W. and Bradshow,P., “Flapping of a Plane Jet,” Phys. Fluids, Vol.16, pp.354-355, 1973.
[15]Gortari,J.C. and Goldschmidt,V.W., “The Apparent Flapping Motion of a Turbulent Plane Jet –Further Experimental Results,” J. Fluids Eng., Vol.103, pp.119-126, 1981.
[16]Antonia,R.A., Chambers,A.J., Britz,D., and Browne,L.W.B., 1986, “Organized Structures in a Turbulent Jet: Topology and Contribution to Momentum and Heat Transport,” J. Fluid Mech., Vol.172, pp.211- 229.
[17]Oler,J.W. and Goldschmidt,V.W., 1980, “Interface Crossing Frequency as a Self-preserving Flow Variable in a Turbulent Plane Jet,” Phys. Fluids, Vol.23, pp.19-21.
[18]Mumford,J.C., 1982, “The Structure of the large Eddies in Fully Developed Turbulent Shear Flows, Part 1. The Plane Jet,” J. Fluid Mech., Vol.118, pp.241-268.
[19]Oler,J.W. and Goldschmidt,V.W., 1982, “A Vortex-street Model of the Flow in the Similarity Region of a Two-dimensional Free Turbulent,” J. Fluid Mech., Vol.123, pp.523-535.
[20]Rayleigh,J.W.S., The Theory of Sound, Vol. II, 2nd ed., Macmillan, London, pp.394-396, 1896.
[21]Stern,M.E. and Voropayev,S.I., “Formation of Vorticity Fronts in Shear Flow,” Phys. Fluids, Vol.27, pp.848-855, 1984.
[22]Atassi,O.V. and Lueptow,R.M., “A model of Flapping Motion in a Plane Jet,” European Journal of Mechanics B/Fluids, Vol.21, pp.171-183, 2002.
[23]Ho,C.M. and Hsiao,F.B., “Evolution of coherent structures in a lip jet,” IUTAM Symposium on Structure of Complex Turbulent Shear Flow, Marseille/France, Spring-Verlag, pp.121-136, 1982.
[24]Huang,J.M., “On the Evolution of Instabilities and Vortex Interaction Processes in the developing region of a Plane Jet,” Ph.D dissertation, Institute of Aeronautics and Astronautics, National Cheng Kung University, Taiwan, R.O.C., 1989.