GAO Zeming, SHAO Xueming, WANG Jiading, et al. Aerodynamic characteristics and vortex ring features of propeller in vertical descent[J]. 2025, 43(1): 1-11.
GAO Zeming, SHAO Xueming, WANG Jiading, et al. Aerodynamic characteristics and vortex ring features of propeller in vertical descent[J]. 2025, 43(1): 1-11.DOI: 10.7638/kqdlxxb-2024.0009.
Aerodynamic characteristics and vortex ring features of propeller in vertical descent
VVPM),对APC thin electric 10X7 螺旋桨在不同垂直下降率下的气动特性和涡环特征开展研究。结果表明:螺旋桨气动特性容易受到下降率的影响,当下降率增加时,拉力呈现先略增大再减小后增大的趋势,同时尾迹压缩效应逐渐增强,涡环中心逐渐上移。在此过程中,涡环先后经历了悬停状态、涡环前期、涡环初期、深度涡环和类风车流动状态,涡环特征从管状螺旋下洗涡逐渐演变成螺旋涡与环形涡并存,再到完全涡环结构,最后涡系结构移动至桨盘上方。涡场拓扑结构的演变直接影响螺旋桨的气动特性,当桨盘附近尾迹为管状螺旋涡结构时,螺旋桨气动特性变化不明显;随着下降率的增加,逐渐演变出的环形涡会严重影响螺旋桨的气动特性,表现为拉力骤降,尾迹压缩效应增强,回流区包裹桨盘;随着下降率进一步增加,涡系结构到达桨盘上方,螺旋桨进入类风车状态,气动力逐渐增大。
Abstract
Propellers are susceptible to entering the perilous vortex ring state during vertical descent
a phenomenon that results in complex aerodynamic characteristics that remain incompletely understood. utilizing the viscous vortex particle method (VVPM)
a thorough investigation was conducted on the aerodynamic characteristics and vortex ring features of the APC thin electric 10X7 propeller at different vertical descent rates. Results show that the propeller's aerodynamic characteristics are highly susceptible to changes in the descent rate. Specifically
as the vertical descent rate increases
the thrust initially experiences a slight increase
followed by a decrease
and ultimately a subsequent increase. Concurrently
the wake compression effect becomes progressively more pronounced
and the vortex ring center gradually shifts upwards. During this process
the vortex ring state transitions sequentially from hovering to a fully developed state
and ultimately transforms into a windmill-like flow state. The wake fields of the propeller gradually change from tubular helicoidal downwash vortical structures to a coexistence of tubular and toroidal vortical structures
and then to fully toroidal ones
which finally migrate completely to the top of the propeller disk. Such a topological evolution of the vortex field has a direct impact on the propeller's aerodynamic characteristics. Tubular helicoidal vortical structures exert negligible influence
while toroidal vortical structures have a significant impact as the descent rate increases
manifested in a sudden thrust decrease
the enhancement of the wake compression effect
the encirclement of propeller discs by backflows
and an increased aerodynamic force.
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references
LEISHMAN J G, BAGAI A . Challenges in understanding the vortex dynamics of helicopter rotor wakes[J ] . AIAA Journal, 1998 , 36 : 1130 − 1140 .
WANG S C. Aerodynamics of helicopter[M]. Beijing: Aviation Industry Press, 1985: 135(in Chinese).
LI G H. Study of high resolution numerical method for helicopter rotor in vortex ring state[D]. Shanghai: Shanghai Jiao Tong University, 2018: 20-25(in Chinese).
MEIJER DREES I J, HENDAL I W P . Airflow patterns in the neighbourhood of helicopter rotors: A description of some smoke tests carried out in a wind tunnel at Amsterdam[J ] . Aircraft Engineering and Aerospace Technology, 1951 , 23 ( 4 ): 107 − 111 .
WASHIZU K, AZUMA A, KOO J, et al. Experimental study on the unsteady aerodynamics of a model helicopter rotor operating in the vortex ring state[C]//Symposium on Structural Dynamics and Aeroelasticity. Boston, MA: AIAA, 1965.
GREEN R B, GILLIES E A, BROWN R E . The flow field around a rotor in axial descent[J ] . Journal of Fluid Mechanics, 2005 , 534 : 237 − 261 .
XIN H, GAO Z . Determination of boundary envelope of helicopter vortex ring area[J ] . Aerodynamic Experiment and Measurement Control, 1996 , 10 ( 1 ): 14 − 19 (in Chinese).
MA H R, MU Z T, LI H W, et al . Revised calculation method f or helicopter vortex-ring state boundary based on flight attitude[J ] . Acta Aerodynamica Sinica, 2018 , 36 ( 1 ): 31 − 34 (in Chinese).
LEISHMAN J G, BHAGWAT M J, ANANTHAN S . The vortex ring state as a spatially and temporally developing wake instability[J ] . Journal of the American Helicopter Society, 2004 , 49 ( 2 ): 160 − 175 .
LI P, CHEN R L . Rotor tip vortex model and its effect on free-vortex wake analysis[J ] . Acta Aeronautica et Astronautica Sinica, 2010 , 31 ( 8 ): 1517 − 1523 (in Chinese).
DZIUBINSKI A, STALEWSKI W. Vortex ring state simulation using actuator disc[C]//ECMS 2007 Proceedings, ECMS, 2007.
GRZEGORCZYK K . Analysis of the influence of helicopter descent velocity changes on the phenomenon of vortex ring state[J ] . Advances in Science and Technology – Research Journal, 2013 , 7 ( 17 ): 35 − 41 .
WANG J J, CHEN R L, WANG Z J, et al . Numerical simulation and mathematical modeling of vortex ring state of Tiltrotor aircraft[J ] . Journal of Harbin Institute of Technology, 2023 , 55 ( 4 ): 35 − 43 (in Chinese).
MIMEAU C, MORTAZAVI I . A review of vortex methods and their applications: From creation to recent advances[J ] . Fluids, 2021 , 6 ( 2 ): 68 .
WANG L Q, HE L, XU G H, et al . Investigation of helicopter rotor aeroacoustic characteristics in vortex ring state[J ] . Acta Aerodynamica Sinica, 2022 , 40 ( 6 ): 83 − 91 (in Chinese).
ZANOTTI A, ALGAROTTI D . Aerodynamic interaction between tandem overlapping propellers in eVTOL airplane mode flight condition[J ] . Aerospace Science and Technology, 2022 , 124 : 107518 .
HE C J, ZHAO J G . Modeling rotor wake dynamics with viscous vortex particle method[J ] . AIAA Journal, 2009 , 47 ( 4 ): 902 − 915 .
WEI P, SHI Y J, XU G H, et al . Numerical method for simulating rotor flow field based upon viscous vortex model[J ] . Acta Aeronautica et Astronautica Sinica, 2012 , 33 ( 5 ): 771 − 780 (in Chinese).
LEE H, LEE D J . Rotor interactional effects on aerodynamic and noise characteristics of a small multirotor unmanned aerial vehicle[J ] . Physics of Fluids, 2020 , 32 ( 4 ): 047107 .
CARADONNA F X, TUNG C. Experimental and analytical studies of a model helicopter rotor in hover: NASA-TM-81232[R]. 1980.
MCCRINK M H, GREGORY J W . Blade element momentum modeling of low-reynolds electric propulsion systems[J ] . Journal of Aircraft, 2017 , 54 ( 1 ): 163 − 176 .