
1. 航天工程大学 宇航科学与技术系,北京,101416
2. 空气动力学国家重点实验室,绵阳,621000
3. 陆军工程大学 爆炸冲击防灾减灾国家重点实验室,南京,210007
Published:2021
移动端阅览
王皓田, 朱杨柱, 车学科, 等. S1223翼型低雷诺数下分离泡及气动特性[J]. 空气动力学学报, 2021, 39(3): 90−98.
WANG Haotian, ZHU Yangzhu, CHE Xueke, et al. Separation bubble and aerodynamic characteristics of S1223 airfoil at low Reynolds numbers[J]. 2021, 39(3): 90-98.
王皓田, 朱杨柱, 车学科, 等. S1223翼型低雷诺数下分离泡及气动特性[J]. 空气动力学学报, 2021, 39(3): 90−98. DOI: 10.7638/kqdlxxb-2020.0075
WANG Haotian, ZHU Yangzhu, CHE Xueke, et al. Separation bubble and aerodynamic characteristics of S1223 airfoil at low Reynolds numbers[J]. 2021, 39(3): 90-98. DOI: 10.7638/kqdlxxb-2020.0075.
采用表面测压技术,测量了低雷诺数下(
Re
= 6.0×10
4
、1.0×10
5
、2.0×10
5
) S1223翼型的表面压力分布,通过时均化处理及瞬态处理方法,分别获得了翼型稳态和瞬态压力系数、升力系数,分析了流场结构随雷诺数及攻角的变化规律,研究了雷诺数及攻角对翼型升力的影响机理。结果表明,从时均升力系数随攻角的变化规律来看,S1223翼型在低雷诺数下存在“静态滞回”效应。攻角由负逐渐增大至0°时,下翼面由完全分离转变为出现层流分离泡,随后分离泡逐渐减小直至消失,导致升力系数斜率呈现随攻角逐渐增大的非线性现象。当攻角超过临界攻角后,不同雷诺数下翼型流场结构随攻角的变化规律存在本质不同,
Re
= 6.0×10
4
和1.0×10
5
时,翼型周围流场迅速发生大范围流动分离,升力系数迅速减小;而
Re
= 2.0×10
5
时,上翼面周期性生成短泡,引发低频振荡现象,升力系数呈现准周期性变化,
α
= 16°时上翼面时均流场呈现40%弦长的长泡结构。
The surface pressure distribution of the S1223 airfoil at low Reynolds numbers (
Re
= 6.0×10
4
1.0×10
5
and 2.0×10
5
) was measured using the surface pressure measurement technique. Both time-averaging and transient processing methods were used to obtain the steady and transient pressure/lift coefficients on the airfoil. Combined with the flow structure analysis
the influence mechanism of the Reynolds number and the angle of attack on the lift of th
e airfoil was studied. According to the variation of time averaged lift coefficient with the angle of attack
S1223 airfoil exibits a "static hysteresis" effect at low Reynolds numbers. The results show that under negative angles of attack
the lift coefficient curve shows a nonlinear phenomenon where its slope gradually increases. When the angle of attack is increased from a negative value
the lower wing surface changes from the state of complete separation to that of laminar separation bubbles
then the separation bubbles gradually shrink until disappeared
resulting in the slope of the lift coefficient curve gradually increasing with the angle of attack. When the angle of attack exceeds the stall value
the flow structures on the S1223 airfoil under different Reynolds numbers are essentially different. At
Re
= 6.0×10
4
and 1.0×10
5
the flow field around the airfoil rapidly undergoes large-scale flow separation
and the lift coefficient decreases sharply; at
Re
= 2.0×10
5
short bubbles on the upper wing surface are generated periodically
causing low-frequency oscillations
and the lift coefficient exhibits a quasi-periodic variation. In the meantime
the averaged flow field on the upper wing surface exhibits a long bubble structure with a chord length of 40%.
JONES B M. An experimental study of stalling of the wings[J]. The Aeronautical Journal, 1934, 38(285): 753-770.
GAULT D E. Boundary-layer and stalling characteristics of the NACA 63-009 airfoil section[R]. NACA TN-1894.
GASTER M. The structure and behaviour of laminar separation bubbles[R]. RM 1966-3595.
WONG C W, KURITA S, RINOIE K. Bubble burst control for stall suppression on a NACA 631-012 airfoil[C ] //47th AIAA Aerospace Sciences Meeting including The New Horizons Forum and Aerospace Exposition, Orlando, Florida. Reston, Virginia: AIAA, 2009. doi: 10.2514/6.2009-1111 .
KOCA K, GENÇ M S, AÇıKEL H H, et al. Identification of flow phenomena over NACA 4412 wind turbine airfoil at low Reynolds numbers and role of laminar separation bubble on flow evolution[J]. Energy, 2018, 144: 750-764.DOI: 10.1016/j.energy.2017.12.045.
SHEN X, AVITAL E, PAUL G, et al. Experimental study of surface curvature effects on aerodynamic performance of a low Reynolds number airfoil for use in small wind turbines[J]. Journal of Renewable and Sustainable Energy, 2016, 8(5): 053303.DOI: 10.1063/1.4963236.
WANG S, MI J C. Effect of large turbulence intensity on airfoil load and flow[J]. Acta Aeronautica et Astronautica Sinica, 2011, 32(1): 41-48. (in Chinese).
WU J, WANG J J, LI T. Experimental investigation on low Reynolds number behavior of NACA0012 airfoi[J]. Journal of Experiments in Fluid Mechanics, 2013, 27(6): 32-38. (in Chinese).
ZHU Z B, LIU Q, BAI P. Large eddy simulation method for the laminar separation phenomenon on low Reynolds number airfoils[J]. Acta Aerodynamica Sinica, 2019, 37(06): 915-923. (in Chinese)DOI: 10.7638/kqdlxxb-2018.0025.
BAI P, CUI E J, LI F, et al. Study of the nonlinear lift coefficient of the symmetrical airfoil at low Reynolds number near the 0° angle of attack[J]. Chinese Journal of Theoretical and Applied Mechanics, 2006, 38(1): 1-8. (in Chinese)DOI: 10.3321/j.issn:0459-1879.2006.01.001.
BAI P, CUI E J, ZHOU W J, et al. An implicit method for the pseudo-compressibility incompressible navier-stokes equation[J]. Chinese Journal of Computational Physics, 2005, 22(5): 386-392. (in Chinese)DOI: 10.3969/j.issn.1001-246X.2005.05.002.
BAI P, CUI E J, ZHOU W J, et al. Numerical simulation of laminar separation bubble over 2D airfoil at low Reynolds number[J]. Acta Aerodynamica Sinica, 2006, 24(4): 416-424. (in Chinese)DOI: 10.3969/j.issn.0258-1825.2006.04.004.
BAI P, LI F, ZHAN H L, et al. Study about the non-linear and unsteady laminar separation phenomena around the airfoil at low Reynolds number with low incidence[J]. Scientia Sinica (Physica, Mechanica Astronomica), 2015, 45(2): 46-57. (in Chinese).
MENG X S, YANG Z R, CHEN Q, et al. Laminar separation control at low Reynolds numbers using plasma actuation[J]. Acta Aeronautica et Astronautica Sinica, 2016, 37(7): 2112-2122. (in Chinese)DOI: 10.7527/S1000-6893.2015.0244.
MENG X S, HU H Y, YAN X, et al. Lift improvements using duty-cycled plasma actuation at low Reynolds numbers[J]. Aerospace Science and Technology, 2018, 72: 123-133.DOI: 10.1016/j.ast.2017.10.038.
ALMUTAIRI J H, JONES L E, SANDHAM N D. Intermittent bursting of a laminar separation bubble on an airfoil[J]. AIAA Journal, 2010, 48(2): 414-426.DOI: 10.2514/1.44298.
ALMUTAIRI J, ALQADII, ELJACK E. Large eddy simulation of a NACA-0012 airfoil near stall[R ] //Direct and Large-Eddy Simulaton IX, ERCOFTAC Series 20, 2015. doi: 10.1007/978-3-319-14448-1_49 .
ALMUTAIRI J, ELJACK E, ALQADI I. Dynamics of laminar separation bubble over NACA-0012 airfoil near stall conditions[J]. Aerospace Science and Technology, 2017, 68: 193-203. doi: 10.1016/j.ast.2017.05.015.
ZAMAN K B M Q, MCKINZIE D J, RUMSEY C L. A natural low-frequency oscillation of the flow over an airfoil near stalling conditions[J]. Journal of Fluid Mechanics, 1989, 202: 403-442.DOI: 10.1017/s0022112089001230.
BRAGG M B, HEINRICH D C, BALOW F A, et al. Flow oscillation over an airfoil near stall[J]. AIAA Journal, 1996, 34(1): 199-201.DOI: 10.2514/3.13045.
BROEREN A P, BRAGG M B. Flowfield measurements over an airfoil during natural low-frequency oscillations near stall[J]. AIAA Journal, 1999, 37(1): 130-132.DOI: 10.2514/2.678.
RINOIE K, TAKEMURA N. Oscillating behaviour of laminar separation bubble formed on an aerofoil near stall[J]. The Aeronautical Journal, 2004, 108(1081): 153-163.DOI: 10.1017/s0001924000000063.
SELIG M S, GUGLIELMO J J. High-lift low Reynolds number airfoil design[J]. Journal of Aircraft, 1997, 34(1): 72-79.DOI: 10.2514/2.2137.
LIU P Q, TANG Z H, CHEN Y X, et al. Experimental feasibility assessment of counter-rotating propellers for stratospheric airships[C ] //53rd AIAA Aerospace Sciences Meeting, Kissimmee, Florida. Reston, Virginia: AIAA, 2015. doi: 10.2514/6.2015-1029 .
CHEN Q Y, TIAN X H, CHE X K, et al. Ground experimental method for stratospheric propeller plasma flow control[J]. Journal of Experiments in Fluid Mechanics, 2015(5): 90-96. (in Chinese)DOI: 10.11729/syltlx20140140.
SUDHAKAR S, VENKATAKRISHNAN L, RAMESH O N. The influence of leading-edge tubercles on airfoil performance at low Reynolds numbers[C ] //Proc of the AIAA Scitech 2020 Forum, Orlando, FL. Reston, Virginia: AIAA, 2020. doi: 10.2514/6.2020-2219 .
GUERRERO J E. Aerodynamic performance of cambered heaving airfoils[J]. AIAA Journal, 2010, 48(11): 2694-2698.DOI: 10.2514/1.J050036.
ARANAKE A C, LAKSHMINARAYAN V K, DURAISAMY K. Computational analysis of shrouded wind turbine configurations using a 3-dimensional RANS solver[J]. Renewable Energy, 2015, 75: 818-832.DOI: 10.1016/j.renene.2014.10.049.
GAO J Q, JIANG H W, XIA B, et al. Frequency spectrum analysis on pressure signals of wind caps in a bubbling fluidized bed[J]. Chinese Journal of Power Engineering, 2011, 31(5): 336-341. (in Chinese).
ZHANG F S, GENG Z X, GE Y Z. Fft algorithm with high accuracy for harmonic analysis in power system[J]. Proceedings of the Chinese Society for Electrical Engineering, 1999(3): 63-66. (in Chinese)DOI: 10.3321/j.issn:0258-8013.1999.03.015.
TANI I. Low-speed flows involving bubble separations[J]. Progress in Aerospace Sciences, 1964, 5: 70-103.DOI:10.1016/0376-0421(64)90004-1
0
Views
0
下载量
0
CSCD
Publicity Resources
Related Articles
Related Author
Related Institution
京公网安备11010802024621