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2015 8 41 8 August 2015 Journal of Beijing University of Aeronautics and Astronautics Vol 41 No 8 http bhxb buaa edu cn jbuaa@ buaa edu cn DOI 10 13700 /j bh 1001-5965 2014 0806 * 1 1 1 1 2 1 361005 2 330024 Rayleigh-Ludwig 45 35% ~ 55% Rayleigh-Ludwig - 0 489 0 5 45 55 9% Rayleigh-Ludwig PIV V211 76 A 1001-5965 2015 08-1381-07 International Civil Aviation Organization ICAO 4 2 ~ 3 min 5 1 8 300 2 1983 2000 6-13 130 NASA 20 1 /3 3-4 2014-12-22 2015-04-10 2015-04-16 09 11 www cnki net /kcms /detail /11 2625 V 20150416 0911 001 html 11072206 * 1961 fbao@ xmu edu cn J 2015 41 8 1381-1387 Bao F Liu J S Zhu R et al Control method for aircraft wake vortex based on Rayleigh-Ludwig instability J Journal of Beijing University of Aeronautics and Astronautics 2015 41 8 1381-1387 in Chinese 6

1382 2015 7-9 R- L DLR ONERA R-L 10 DLR F13 11-12 18 13 UCB 19 1 22 UND 20 Vor 23 14-16 15-16 16 2 24-25 17-19 2 1 Rayleigh-Ludwieg Rayleigh-Ludwig 20 R-L R-L 2 1 21 Γ 1 > 0 Γ 2 < 0 Γ 1 Γ 2 Fig 1 b 1 b 2 21 1 Classification chart of four-vortex wake system 21 a r 1 /4 2 Fig 2 Schematic of experimental model and four-vortex wake system tailored by the model

8 1383 GO436B 80 mm b = 200 mm 0 75 mm 8 981 736 1 interrogation window 16 16 25% overlap PIV 4 1 Table 1 Shapes and sizes of spoiler /mm a = 40 45 50 55 1 /4 r = 40 45 50 55 PIV Partical Image Velocimetry 3-500 mm 520 mm 4 PIV Fig 4 Coordinate system for PIV measurement region 3 300 m 0 5 mm /s 45 0 4 ~ 0 5 m /s 6 ~ 15 min 10 3 98 10 4 ~ 4 95 10 4 3 2 3 PIV 3 1 baseline α 10 8 6 V 0 4 0 5 m /s 6 3 PIV α = 10 V = 0 5 m /s Fig 3 Xiamen university fluid dynamics and PIV laboratory 30 5 b x /b PIV 45 PIV 2 2 PIV Table 2 Component parameters of PIV system Nd YAG 15 W CCD SpeedSense9040 1 600 1 200 AF VR Zoom-Nikkor = 80 ~ 400 mm Dynamic Studio V3 31 Al 2 O 3 = 5 μm 5 30 Fig 5 Development of primary vortex in 30 wingspans without spoiler

1384 2015 30 8 PIV Dynamicstudio ω 1 v u x y V S Г 2 A Γ i /Γ 1 i Γ i 7 Γ 1 Fig 7 Circulation variation of primary vortex ω = v x - u 1 respecting to wingspan without spoiler y Γ L = V ds = L ωda 2 A α = 10 V = 0 5 m /s 45 Γ i /Γ 1 6 12 8 Fig 8 Development of primary vortex with spoiler 45 36 ~ 45 0 92 5 8 1 2 6 45 Fig 6 Circulation development curve of primary vortex in 24 45 wingspans without spoiler 9 6 45 Γ i /Γ 1 ω 7 45 5 14 3 2 R-L 16 ~ 17 R-L 45 α = 10 V = 0 5 m /s Γ i /Γ 1 10

8 1385 45 a = 50 mm 5 55 9% 21 0 42 Fig 9 Fig 10 10 45 Circulation development curve of primary vortex in 45 wingspans with spoiler α = 10 V = 0 5 m /s 45 Γ i /Γ 1 11 Fig 11 11 Circulation variation of primary vortex respecting to wingspan in four-vortex wake system Γ 2 / - Γ 1 η η - b 2 /b 1 1 r = 50 mm 3 3 Table 3 Relationship between parameters in four-vortex wake system V / m s α / b 2 /b 1 Γ 2 / - Γ 1 η /% η - /% 0 4 8 0 4 0 406 37 30 10 0 4 0 367 36 80 a = 40 mm 6 0 4 0 414 41 30 42 0 9 0 5 8 0 4 0 373 45 80 Vortical contour of primary vortex with spoiler 10 0 4 0 376 48 60 6 0 45 0 411 47 60 0 4 8 0 45 0 391 43 80 a = 45 mm 10 0 45 0 38 49 70 6 0 45 0 388 46 50 48 1 0 5 8 0 45 0 402 49 80 10 0 45 0 402 51 20 6 0 5 0 409 53 10 0 4 8 0 5 0 440 40 20 a = 50 mm 10 0 5 0 491 49 40 6 0 5 0 443 50 70 49 7 0 5 8 0 5 0 467 48 80 10 0 5 0 489 55 90 a = 55 mm r = 50 mm 0 4 0 5 0 4 0 5 6 0 55 0 479 51 30 8 0 55 0 482 47 70 10 0 55 0 472 53 40 6 0 55 0 439 50 80 8 0 55 0 465 53 80 10 0 55 0 469 55 10 6 0 5 0 423 44 00 8 0 5 0 498 43 70 10 0 5 0 475 36 90 6 0 5 0 425 40 70 8 0 5 0 488 47 20 10 0 5 0 455 44 20 52 0 42 8

1386 2015 40 mm a 50 mm 0 367 Γ 2 / - Γ 1 0 491 a 55% Γ 2 / - Γ 1 0 5 b 2 /b 1 0 55 0 44 Γ 2 / - Γ 1 0 49 Γ 2 / - Γ 1 η R-L a = 50 mm r = 50 mm 3 12 3 Veillette P R Data show that U S wake-turbulence accidents are most frequent at low altitude and during approach and landing J Flight Safety Digest 2002 21 3-4 1-47 4 Holz pfel F Sensitivity analysis of the effects of aircraft and environmental parameters on aircraft eake vortex trajectories and lifetimes AIAA-2013-0363 R Reston AIAA 2013 12 Fig 12 Distribution of effective parameters 5 Borer N K Barrows T M Levine D M et al Formation airdrop combinations in four-vortex wake system classification chart scaling effects on aircraft wake vortex formation and interaction AIAA-2013-0361 R Reston AIAA 2013 12 6 Burnham D C Hallock J N Decay characteristics of wake vortices from jet transport aircraft J Journal of Aircraft 2012 29 50 1 82-87 45 50% 7 Stewart E C A study of the interaction between a wake vortex 0 5 b 2 /b 1 0 55 0 44 Γ 2 / - Γ 1 0 49 AIAA 1993 b 2 /b 1 = 0 5 Γ 2 / - Γ 1 0 489 4 PIV R-L 1 2 2012 R-L 3 R-L 10 ~ 20 4 a = r 398-404 5 45 References 1 Burnham D C Hallock J N Decay characteristics of wake vortices from jet transport aircraft J Journal of Aircraft 2012 50 1 82-87 2 Dacles-Mariani J Hafez M Kwak D Prediction of wake-vortex flow inthenear-and intermediate-fields behind wings AIAA- 1997-0040 R Reston AIAA 1997 and an encountering airplane AIAA-1993-3642 R Reston 8 Perry R B Hinton D A Stuever R A NASA wake vortex research for aircraft spacing AIAA-1997-0057 R Reston AIAA 1997 9 Zheng Z C Xu Y Wilson D K Behaviors of vortex wake in random atmospheric turbulence J Journal of Aircraft 2009 46 6 2139-2144 10 Harris M Young R I K pp F et al Wake vortex detection and monitoring J Aerospace Science and Technology 2002 6 5 325-331 11 Holz pfel F Frech M Gerz T et al Aircraft wake vortex scenarios simulation package-wakescene J Aerospace Science and Technology 2009 13 1 1-11 12 Kauertz S Holz pfel F Kladetzke J Wake vortex encounter risk assessment for crosswind departures J Journal of Aircraft 49 1 281-291 13 Stephan A Holz pfel F Misaka T Aircraft wake-vortex decay in ground proximity-physical mechanisms and artificial enhancement J Journal of Aircraft 2013 50 4 1250-1260 14 Rennich S C Lele S K Method for accelerating the destruction of aircraft wake vortices J Journal of Aircraft 1999 36 2

8 15 Bao F Vollmers H Mattner H Experimental study on controlling wake vortex in water towing tank C Proceedings of 20th 1387 International Congress on Instrumentation in Aerospace Simula- 21 Babie B M Nelson R C An experimental investigation of bending wave instability modes in a generic four-vortex wake J 16 Robert Konrath Physics of Fluids 2010 22 7 1-15 tion Facilities Piscataway NJ IEEE Press 2003 214-223 J 2010 31 5 899-908 22 Quackenbush T R Boschitsch A H Bilanin A J Computational Huang S Q Shen G X Konrath R et al Experimental investiga- and experimental studies in multipair wake vortex instabilities tion of influence of jets on aircraft wake vortices J Acta Aeronautica et Astronautica Sinica 2010 31 5 899-908 in Chinese 17 Urbatzka E Wilken D Estimating runway capacities of German airports J Transportation Planning Technology 1997 20 2 103-129 18 Fabre D Jacquin L Stability of a four-vortex aircraft wake model J Physics of Fluids 2000 12 10 2438-2443 19 Rennich S C Lelet S K Method for accelerating the destruction of aircraft wake vortices J Journal of Aircraft 1999 36 2 398-404 20 Ortega J M Bristol R L Savas Experimental study of the instability of unequal-strength counter-rotating vortex pairs J Journal of Fluid Mechanics 2003 474 35-84 AIAA-2013-3190 R Reston AIAA 2013 23 Jacquin L Fabre D Sipp D et al Instability and unsteadiness of aircraft wake vortices J Aerospace Science and Technology 2003 7 8 577-593 24 Rayleigh-Ludwieg J 2013 27 2 24-30 Liu Z R Zhu R Dual wingtips vortexes Rayleigh-Ludwieg instability experimental research J Journal of Experiments in Fluid Mechanics 2013 27 2 24-30 in Chinese 25 He Y Yang J W Bao F Wake vortex control using modified flaps J Applied Mechanics and Materials 2013 365 827-834 Control method for aircraft wake vortex based on Rayleigh-Ludwig instability BAO Feng * 1 LIU Jinsheng 1 ZHU Rui 1 JIANG Jianhua 1 WANG Junwei 2 1 School of Physics and Mechanical & Electrical Engineering Xiamen University Xiamen 361005 China 2 Jiangxi Hongdu Aviation Industry Co Ltd Nanchang 330024 China Abstract The aircraft wake vortex is an inherent flow phenomenon due to the lift generation mechanism which has a negative impact on the flight safety By adding a set of specially designed spoiler a rectangular wing was designed to generate a pair of weaker vortices which had different sizes and opposite direction compared to main wing vortices thereby constructing a self-destructive four-vortex wake system to induce Rayleigh-Ludwig instability Under different experimental conditions in terms of changing the size or shape of the spoiler towing speed and angle of attack the wake vortex development of the test model that both with and without spoiler as well as the circulation analysis were acquired particle image velocimetry PIV measurements under the low Reynolds number The study demonstrates that the decrease in circulation was 35% to 55% in 45 wingspans when spoilers are introduced whereas the counterpart of the baseline airfoil without spoilers is nearly kept steadily which reveal the application possibility of Rayleigh-Ludwig instability in alleviating the wake vortex As the initial circulation ratio equals to - 0 489 and the initial distance ratio is 0 5 the circulation of the primary vortex reduce most significantly 55 9% in 45 wingspans Results would provide a scheme in the design of airfoils with weaker vortices Key words aircraft wake vortex Rayleigh-Ludwig instability particle image velocimetry PIV spoiler low Reynolds number