ACTA AERONAUTICAET ASTRONAUTICA SINICA >
Interactive aerodynamic characteristics of canard rotor wing aircraft in helicopter forward flight
Received date: 2016-01-13
Revised date: 2016-03-14
Online published: 2016-03-23
Supported by
National Natural Science Foundation of China (11372254)
Compared with the traditional helicopter, the aerodynamic interaction of rotor wing, fuselage, canard and horizontal tail of canard rotor wing (CRW) aircraft in forward flight is severer. In order to get better understanding of the unsteady aerodynamic interaction, the moving structural chimera grid is used to model the moving rotor and three-dimensional unsteady Reynolds averaged Navier-Stokes (URANS) equations are solved to simulate the flow fields of rotor in forward flight. The traditional helicopter's rotor-body interaction model is computed first to validate the method. Then the analyses on rotor wing/fuselage/canard/horizontal tail/vertical tail interactive flow field for an unmanned CRW aircraft in helicopter forward flight are given using the present method. The variations of unsteady aerodynamic forces and moments of the rotor-wing, fuselage, canard, horizontal tail and vertical tail with respect to the rotor azimuth are obtained. The result shows that the fuselage and other components have little effect on the rotor wing, resulting in a slight increase in thrust; the rotor wing has almost no impact on the aerodynamics of canard and vertical tail, but does have strong interference on fuselage and horizontal tail. The horizontal tail produces large vertical force and nose-up pitching moment as the forward flight speed increases, to which great attention should be paid. The research could provide some guidance for the design of a CRW aircraft.
SUN Wei , GAO Zhenghong , JIANG Jiechu . Interactive aerodynamic characteristics of canard rotor wing aircraft in helicopter forward flight[J]. ACTA AERONAUTICAET ASTRONAUTICA SINICA, 2016 , 37(8) : 2498 -2506 . DOI: 10.7527/S1000-6893.2016.0092
[1] MITCHELL C A, VOGEL B J. The canard rotor wing (CRW) aircraft-a new way to fly:AIAA-2003-2571[R]. Reston:AIAA, 2003.
[2] 邓阳平, 高正红, 詹浩. 鸭式旋翼/机翼飞机的技术发展及其关键技术[J]. 飞行力学, 2006, 24(3):1-4 DENG Y P, GAO Z H, ZHAN H. Development and key technologies of the CRW[J]. Flight Dynamics, 2006, 24(3):1-4(in Chinese).
[3] 孙威, 高正红, 黄江涛, 等. 旋转机翼悬停气动特性研究[J]. 空气动力学学报, 2015, 33(2):232-238. SUN W, GAO Z H, HUANG J T, et al. Aerodynamic characteristics of hovering rotor/wing[J]. Acta Aerodynamica Sinica, 2015, 33(2):232-238(in Chinese).
[4] SUN W, GAO Z H, DU Y M, et al. Mechanism of unconventional aerodynamic characteristics of an elliptic airfoil[J]. Chinese Journal of Aeronautics, 2015, 28(3):687-694.
[5] 邓阳平, 高正红, 詹浩. 鸭式旋翼/机翼飞机悬停及小速度前飞气动干扰实验研究[J]. 实验力学, 2009,24(6):563-567. DENG Y P, GAO Z H, ZHAN H. Experimental investigation on aerodynamic interactions of canard rotor/wing aircraft in hover and low speed forward flight[J]. Journal of Experimental Mechanics, 2009, 24(6):563-567(in Chinese).
[6] MCKENNA J T. One step beyond[J]. Rotor & Wing, 2007, 41(2):54-56.
[7] THOMPSON T L, SMITH R L, HELWANI M, et al. Wind tunnel test results for a Canard Rotor/Wing aircraft configuration[C]//57th Annual Forum of American Helicopter Society. Alexandria, VA:American Helicopter Society Inc., 2001, 57(2):1431-1443.
[8] 孙威, 高正红. 旋转机翼飞机旋翼/机身干扰流场数值计算分析[J]. 飞行力学, 2011, 29(6):4-8. SUN W, GAO Z H. Numerical computation and analysis on rotor/fuselage interactive flow field for rotor wing plane[J]. Flight Dynamics, 2011, 29(6):4-8(in Chinese).
[9] SAEID N R, GENESH R, THOMAS L T. Simulation of unsteady aerodynamics of the unmanned CRW dragonfly aircraft hovering near the ground[C]//The AHS International Specialists' Meeting on Unmanned Rotorcraft. Alexandria, VA:American Helicopter Society Inc., 2005:439-459.
[10] RAJAGOPALAN R G, FANUCCI J B. Finite difference model for vertical axis wind turbines[J]. Journal of Propulsion and Power,1985, 1(6):432-436.
[11] LI Y B, MA D L. Numerical simulation of rotor-aerodynamic surface interaction in hover using moving chimera grid[J]. Chinese Journal of Aeronautics, 2012, 25(3):342-348.
[12] YOON S, JAMESON A. Lower-upper symmetric-Gauss-seidel method for the Euler and Navier-Stokes equations[J]. AIAA Journal, 1988, 26(9):1025-1026.
[13] ROE P L. Approximate riemann solvers, parameter vectors, and difference schemes[J]. Journal of Computational Physics, 1997, 135(2):250-258.
[14] SPALART P R, ALLMARAS S R. A one equation turbulence model for aerodynamic flows:AIAA-1992-0439[R]. Reston:AIAA, 1992.
[15] WEISS J M, SMITH W A. Preconditioning applied to variable and constant density flow[J]. AIAA Journal, 1995, 33(11):2050-2057.
[16] MINECK R E, GORTTON S A. Steady and periodic pressure measurements on a generic helicopter fuselage model in the presence of a rotor:NASA/TM-2000-210286[R]. Washington D.C.:NASA, 2000.
[17] O'BRIEN D M, JR. Analysis of computational modeling techniques for complete rotorcraft configurations[D]. Atlanta:Georgia Institute of Technology, 2006:121-125.
[18] PARK Y M, NAM H J, KOWN O J. Simulation of unsteady rotor-fuselage interactions using unstructured adaptive meshes[C]//59th Annual Forum of the American Helicopter Society. Alexandria, VA:American Helicopter Society Inc., 2003:1-11.
[19] TADGHIGHI H. Simulation of rotor-body interactional aerodynamics:an unsteady rotor source distributed disk model[C]//57th Annual Forum of American Helicopter Society. Alexandria, VA:American Helicopter Society Inc., 2001.
[20] CHAFFIN M S, BERRY J D. Helicopter fuselage aerodynamics under a rotor by Navier-Stokes simulation[J]. Journal of American Helicopter Society, 1997, 42(3):235-242.
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