CN108733914A - Transonic airfoil Natural Laminar Flow delay based on artificial neural network turns to twist design method - Google Patents
Transonic airfoil Natural Laminar Flow delay based on artificial neural network turns to twist design method Download PDFInfo
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Abstract
发明属于飞机设计技术领域,具体为一种基于人工神经网络的跨音速翼型自然层流延迟转捩设计方法。本发明的具体步骤如下:(1)利用翼型参数化方法分析翼型的外形,建立翼型参数化表达方式;(2)根据翼型在跨音速巡航流场中的气动特点,提取和跨音速自然层流相关的气动参数;(3)利用人工神经网络技术,实现智能的系统优化;最终输出相应的新翼型数据。本发明方法可使在飞机跨音速巡航飞行下,在(弱)激波‑边界层的复杂流动环境中,实现翼型表面层流区域的扩大,从而延迟层流转捩的发生,实现摩擦阻力减小的目标。由本发明所获得的新的优良跨音速自然层流性能的翼型,可以应用于飞机机翼和发动机短舱剖面的设计优化之中。
The invention belongs to the technical field of aircraft design, and specifically relates to a method for designing a natural laminar flow delay transition of a transonic airfoil based on an artificial neural network. The specific steps of the present invention are as follows: (1) use the airfoil parameterization method to analyze the shape of the airfoil, and establish the airfoil parameterization expression; (2) according to the aerodynamic characteristics of the airfoil in the transonic cruise flow field, extract and transonic Aerodynamic parameters related to natural laminar flow at the speed of sound; (3) Using artificial neural network technology to realize intelligent system optimization; finally output corresponding new airfoil data. The method of the invention can realize the expansion of the laminar flow area on the surface of the airfoil in the complex flow environment of the (weak) shock wave-boundary layer under the transonic cruise flight of the aircraft, thereby delaying the occurrence of the laminar flow transition and realizing the reduction of frictional resistance small goals. The new airfoil with excellent transonic natural laminar flow performance obtained by the invention can be applied to the design optimization of aircraft wings and engine nacelle sections.
Description
技术领域technical field
本发明属于飞机设计技术领域,具体涉及飞机跨音速翼型自然层流延迟转捩设计方法。The invention belongs to the technical field of aircraft design, and in particular relates to a design method for a natural laminar flow delay transition of an aircraft transonic airfoil.
背景技术Background technique
现代民用飞机设计需要满足“四性”,即安全性、经济型、舒适性和环保性。在欧美国家该领域已经具有绝对优势、国际竞争非常激烈、市场准入门槛很高的形势下开展大型客机工程,要求我们重视基础研究,建立雄厚的科研实力和长远的技术储备,形成自主创新和可持续发展能力。The design of modern civil aircraft needs to meet the "four characteristics", namely safety, economy, comfort and environmental protection. Under the situation that European and American countries already have absolute advantages in this field, the international competition is very fierce, and the market entry threshold is very high, we need to pay attention to basic research, establish strong scientific research strength and long-term technical reserves, and form independent innovation and Sustainability.
飞机的阻力直接决定了飞机的经济性和排放。减阻与经济性和环保性密切相关,其中经济性是决定航空公司飞机选购的主要因素,而环保性可能成为未来航空市场的准入条件。大型客机飞行时的流场是决定飞机的气动性能的重要因素。层流层流转捩为湍流是由于附面层失稳和扰动的进一步增长,而附面层不稳定性起源于增长或衰减的小的速度扰动,小速度扰动的增长导致大的振幅,非线性性质,并最终使流动从层流转捩为湍流。在线性不分离的情况下,流体的能量消耗于临界区域的剪切运动,在分离的情况下,则有更大部分的能量还散失于脱边分离后的漩涡运动。Aircraft drag directly determines aircraft economy and emissions. Drag reduction is closely related to economy and environmental protection, among which economy is the main factor that determines the airline's aircraft purchase, and environmental protection may become the access condition of the future aviation market. The flow field of a large passenger aircraft is an important factor determining the aerodynamic performance of the aircraft. The transition from laminar flow to turbulent flow is due to boundary layer instability and further growth of disturbances, while boundary layer instability originates from small velocity disturbances that grow or decay, and the growth of small velocity disturbances leads to large amplitude, non-linear properties, and eventually the flow transitions from laminar to turbulent. In the case of linear non-separation, the energy of the fluid is consumed in the shearing motion in the critical region, and in the case of separation, a larger part of the energy is lost in the vortex motion after the edge separation.
飞机表面流场种层流和湍流的分布起着比较重要的作用。例如,大型客机飞行的流场阻力包括摩擦阻力、诱导阻力和激波阻力等,尽可能延迟转捩的发生,即扩大模型表面上层流流动的区域,减小湍流浸润面积,是流动控制减小摩擦阻力的有效手段。又如,湍流区域的减小,会使得湍流激励噪声也将随之降低。这些例子均说明了层流/湍流的分布对于飞机的气动性能的关键作用,同时也说明了飞机机翼延迟转捩技术的迫切的需求。The distribution of laminar flow and turbulent flow in the flow field on the surface of the aircraft plays a more important role. For example, the flow field resistance of a large airliner flight includes frictional resistance, induced resistance, and shock wave resistance, etc., delaying the occurrence of transition as much as possible, that is, expanding the area of laminar flow on the surface of the model, reducing the area of turbulent flow infiltration, and reducing the flow control. Effective means of frictional resistance. As another example, the reduction of the turbulent flow area will reduce the turbulent flow excitation noise. These examples all illustrate the key role of the distribution of laminar/turbulent flow on the aerodynamic performance of the aircraft, and also illustrate the urgent need for the delayed transition technology of the aircraft wing.
目前,常规的飞机的设计已经处在瓶颈阶段,先进的理论和方法正在给大型客机的研制带来深刻的变革和进步,为提高民用飞机“四性”,欧美等国已开展了一系列的前瞻性研究。欧洲在其民用航空2020远景规划中提出了所谓“绿色飞机挑战”,主要目标包括:在2020年将NOX排放减少80%,CO2排量减少50%(燃油消耗减半),事故概率减半,飞机可感受噪音减半(将机场边界处的噪声降低到65dB),航空运行周转效率大幅提高。NASA在1994~2001年实施了先进亚音速飞机技术(AST)研究计划后,在2001年又启动了安静飞机技术(QAT)研究计划,计划较1997年的水平进一步降低飞机噪声5dB,未来目标是在25年内降低20dB。At present, the design of conventional aircraft is already at the bottleneck stage, and advanced theories and methods are bringing profound changes and progress to the development of large passenger aircraft. In order to improve the "four characteristics" of civil aircraft, Europe, the United States and other countries have launched a series of prospective study. Europe has put forward the so-called "green aircraft challenge" in its civil aviation 2020 long-term plan. The main goals include: reducing NOX emissions by 80%, CO2 emissions by 50% (fuel consumption is halved), and accident probability by 2020. Aircraft can feel that the noise is halved (the noise at the airport boundary is reduced to 65dB), and the turnover efficiency of aviation operations is greatly improved. After NASA implemented the Advanced Subsonic Aircraft Technology (AST) research program from 1994 to 2001, it launched the Quiet Aircraft Technology (QAT) research program in 2001. It plans to further reduce aircraft noise by 5dB compared with the level in 1997. The future goal is 20dB reduction in 25 years.
为了使我国能尽快形成有国际竞争力的大型客机产业,非常有必要加强相关基础科学问题的研究,夯实大型客机研制的基础,开展新型研究方法,构建自主创新能力,在核心技术上实现可持续发展,服务现实和未来航空的需求。In order to enable my country to form a large passenger aircraft industry with international competitiveness as soon as possible, it is very necessary to strengthen research on relevant basic scientific issues, consolidate the foundation for the development of large passenger aircraft, develop new research methods, build independent innovation capabilities, and achieve sustainable development in core technologies. Development, serving the needs of reality and future aviation.
发明内容Contents of the invention
本发明的目的在于提供一种飞机跨音速翼型自然层流延迟转捩设计方法,使在飞机跨音速巡航飞行下,在(弱)激波-边界层的复杂流动环境中,实现翼型表面层流区域的扩大,从而延迟层流转捩的发生,实现摩擦阻力减小的目标。The object of the present invention is to provide a kind of aircraft transonic airfoil natural laminar delay transition design method, make under the aircraft transonic cruise flight, in the complex flow environment of (weak) shock wave-boundary layer, realize airfoil surface The expansion of the laminar flow area delays the occurrence of laminar flow transition and achieves the goal of reducing frictional resistance.
本发明提出的飞机跨音速翼型自然层流延迟转捩设计方法,是基于人工神经网络技术的,具体步骤如下:The aircraft transonic airfoil natural laminar delay transition design method proposed by the present invention is based on artificial neural network technology, and the specific steps are as follows:
(1)利用翼型参数化方法分析翼型的外形,建立翼型参数化表达方式;(1) Analyze the shape of the airfoil by using the airfoil parameterization method, and establish the parametric expression method of the airfoil;
采用PARSEC参数化方法(Sobieczky H.Parametric airfoils and wings[M]//Recent Development of Aerodynamic Design Methodologies.Vieweg+Teubner Verlag,1999:71-87.)描述飞机翼型,建立飞机翼型表达方式,即以如下11个PARSEC参数:前缘半径rle,上/下翼面最大厚度Xup和Xlo,上/下翼面最大厚度对应位置Zup和Zlo,上/下翼面顶点曲率Zxxup和Zxxlo,后缘宽度△ZTE,后缘垂直高度ZTE,后缘楔角βTE,后缘方向角αTE,以模拟翼型几何状况。PARSEC参数化方法很简练地把流动特征和翼型几何特征关联起来,对于设计和研究均有着很大的益处。由此,上翼面和下翼面曲线参数化表达式为式(1)所示:Using the PARSEC parameterization method (Sobieczky H.Parametric airfoils and wings[M]//Recent Development of Aerodynamic Design Methodologies. Vieweg+Teubner Verlag, 1999:71-87.) to describe the aircraft airfoil and establish the expression of the aircraft airfoil, namely Take the following 11 PARSEC parameters: leading edge radius r le , maximum thickness X up and X lo of the upper/lower airfoil, corresponding positions Z up and Z lo of the maximum thickness of the upper/lower airfoil, apex curvature Z xxup of the upper/lower airfoil and Z xxlo , trailing edge width △ Z TE , trailing edge vertical height Z TE , trailing edge wedge angle β TE , trailing edge direction angle α TE , to simulate airfoil geometry. The PARSEC parameterization method succinctly associates the flow characteristics with the airfoil geometric characteristics, which is of great benefit to both design and research. Therefore, the parametric expressions of the upper and lower airfoil curves are shown in formula (1):
an(n=1,2,…,6)为多项式系数。对于上翼面,系数an由矩阵方程(2)给出:a n (n=1,2,...,6) are polynomial coefficients. For the upper airfoil, the coefficient a n is given by the matrix equation (2):
对于下翼面,系数an由矩阵方程(3)给出,其和上翼面类似,即将表征上翼面构型特征量的参数换成下翼面相对应的参数:For the lower airfoil, the coefficient a n is given by the matrix equation (3), which is similar to the upper airfoil, that is, the parameters representing the configuration characteristics of the upper airfoil are replaced by the corresponding parameters of the lower airfoil:
获得拟合系数,便可以建立几何参数与实际翼型外形的联系。其中xup为上翼面各个点横坐标,xte为翼面尾缘处的横坐标。By obtaining the fitting coefficient, the relationship between the geometric parameters and the actual airfoil shape can be established. Where x up is the abscissa of each point on the upper airfoil, and x te is the abscissa of the trailing edge of the airfoil.
(2)根据翼型在跨音速巡航的流场中的气动特点,提取和跨音速自然层流相关的气动参数;运用流场计算方程进行流场计算并获得层流区域长度的结果。流场求解选用NS方程(Currie,I.G.(1974),Fundamental Mechanics of Fluids,McGraw-Hill,ISBN 0-07-015000-1),采用SST湍流模型(Menter,F.R.(August 1994),"Two-EquationEddy-Viscosity Turbulence Models for Engineering Applications",AIAA Journal,32(8):1598–1605,Bibcode:1994AIAAJ..32.1598M,doi:10.2514/3.12149)。在求解层流-湍流分布的时候应用基于SST湍流模式的间歇因子的γ-Re转捩模型(Langtry R,MenterF.Transition Modeling for General CFD Applications in Aeronautics[M].2015.),如式(4)(5)所示,其中ρ为密度,U为速度,p为压力,γ为湍流间歇因子,Reθt为当地动量雷诺数,μ为分子粘度,μt为根据Boussinesq假设的湍流粘度,Pγ为湍流间歇因子生成项,Eγ为湍流间歇因子耗散项,Uj为j方向的速度(j=1,2,3),σf为经过实验标定的系数,Pθt为动量雷诺数产生项:(2) According to the aerodynamic characteristics of the airfoil in the flow field of transonic cruise, the aerodynamic parameters related to the transonic natural laminar flow are extracted; the flow field calculation equation is used to calculate the flow field and obtain the result of the length of the laminar flow region. The NS equation (Currie, IG (1974), Fundamental Mechanics of Fluids, McGraw-Hill, ISBN 0-07-015000-1) was used to solve the flow field, and the SST turbulence model (Menter, FR (August 1994), "Two-EquationEddy -Viscosity Turbulence Models for Engineering Applications", AIAA Journal, 32(8):1598–1605, Bibcode:1994AIAAJ..32.1598M, doi:10.2514/3.12149). When solving the laminar-turbulent flow distribution, the γ-Re transition model based on the intermittent factor of the SST turbulence model (Langtry R, MenterF. Transition Modeling for General CFD Applications in Aeronautics [M]. 2015.), as shown in formula (4 )(5), where ρ is the density, U is the velocity, p is the pressure, γ is the turbulent intermittent factor, Re θt is the local momentum Reynolds number, μ is the molecular viscosity, μ t is the turbulent viscosity assumed by Boussinesq, P γ is the generation item of the turbulent intermittent factor, E γ is the dissipation item of the turbulent intermittent factor, U j is the velocity in the j direction (j=1, 2, 3), σ f is the coefficient calibrated by the experiment, P θt is the momentum Reynolds number Produced items:
通过求解以上方程组获得流场解,得到对应的层流区域长度的气动性能参数。The flow field solution is obtained by solving the above equations, and the corresponding aerodynamic performance parameters of the length of the laminar flow region are obtained.
(3)利用人工神经网络技术,实现智能的系统优化;最终输出相应的新翼型数据,新翼型具备改进的跨音速自然层流特性。(3) Use artificial neural network technology to realize intelligent system optimization; finally output corresponding new airfoil data, and the new airfoil has improved transonic natural laminar flow characteristics.
通过人工神经网络(ANN)算法(Zeidenberg M.Neural networks in artificialintelligence[M].Ellis Horwood,1990.),实现优化设计。关于神经网络的训练方法,采用GRNN算法(Specht D F.A general regression neural network.Neural Networks[J],IEEE Transactions on,1991.2(6):p.568-576.)(经过比较,其目标相关系数水平和网络泛化能力均优于BP算法和RBF算法)。广义回归神经网络(GRNN)是美国学者DonaldF.Specht在1991年提出的,它是径向基神经网络的一种变化形式。GRNN是一种基于非线性回归分析的前馈式神经网络,具有很强的非线性映射能力和柔性网络结构以及高度的容错性和鲁棒性,适用于解决非线性问题.GRNN由四层构成,分别为输入层,模式层,求和层和输出层。The optimal design is realized through the artificial neural network (ANN) algorithm (Zeidenberg M. Neural networks in artificial intelligence [M]. Ellis Horwood, 1990.). Regarding the training method of the neural network, the GRNN algorithm (Specht D F.A general regression neural network. Neural Networks[J], IEEE Transactions on, 1991.2(6): p.568-576.) was used (after comparison, the level of the target correlation coefficient and network generalization ability are better than BP algorithm and RBF algorithm). Generalized regression neural network (GRNN) was proposed by American scholar Donald F. Specht in 1991. It is a variation of radial basis neural network. GRNN is a feed-forward neural network based on nonlinear regression analysis. It has strong nonlinear mapping ability, flexible network structure, and high fault tolerance and robustness. It is suitable for solving nonlinear problems. GRNN consists of four layers. , are the input layer, model layer, summation layer and output layer, respectively.
这里的优化过程为迭代过程的。在一次优化步骤中,首先,根据初始待优化翼型,分析得到对应的11个PARSEC几何参数;通过拉丁超立方采样技术(Owen,A.B.(1992)."Orthogonal arrays for computer experiments,integration and visualization".Statistica Sinica.2:439–452.)进行参数扰动,获得一系列的新的翼型对应几何参数。每次优化步骤中扰动的范围是逐渐减小的,以期最终收敛到一个优化了的跨音速层流翼型。针对通过参数扰动获得的一系列翼型,运用上面提到的流场计算方程进行流场计算并获得层流区域长度的结果。The optimization process here is an iterative process. In one optimization step, firstly, according to the initial airfoil to be optimized, the corresponding 11 PARSEC geometric parameters are analyzed; through the Latin hypercube sampling technique (Owen, A.B. (1992). "Orthogonal arrays for computer experiments, integration and visualization" .Statistica Sinica.2:439–452.) Perform parameter perturbation to obtain a series of new airfoil corresponding geometric parameters. The perturbation range is gradually reduced in each optimization step in order to eventually converge to an optimized transonic laminar airfoil. For a series of airfoils obtained by parameter perturbation, the flow field calculation equation mentioned above is used to calculate the flow field and obtain the result of the length of the laminar flow region.
在每一次优化步骤中,每个新翼型都有了对应的几何参数和层流区域长度的气动性能参数。本方法采用基于人工神经网络的代理模型建立两者的联系。在训练人工神经网络的时候,输入端为本次优化步骤的各个翼型的气动性能(层流长度),输出端为各个翼型的几何参数。然后进行训练获得代理模型。At each optimization step, each new airfoil has corresponding geometric parameters and aerodynamic performance parameters for the length of the laminar flow region. This method uses an agent model based on artificial neural network to establish the connection between the two. When training the artificial neural network, the input end is the aerodynamic performance (laminar flow length) of each airfoil in this optimization step, and the output end is the geometric parameters of each airfoil. Then train to obtain a proxy model.
接下来进行本次优化步骤的优化,在训练好的人工神经网络中输入一个合适的目标层流区域长度参数,以期获得对应新翼型的几何参数。这里的“合适”主要是说:1.所输入的目标层流区域长度不可过于理想,因为这不符合我们的逐步优化的概念;2.过高的输入会造成新的生成翼型的形状扭曲。Next, the optimization of this optimization step is carried out, and an appropriate target laminar region length parameter is input into the trained artificial neural network, in order to obtain the geometric parameters corresponding to the new airfoil. "Appropriate" here mainly means: 1. The length of the input target laminar flow area should not be too ideal, because it does not conform to our concept of step-by-step optimization; 2. Too high input will cause the shape of the new generated airfoil to be distorted .
合适的输入一般参照本次优化步骤中所参数扰动生成的一系列翼型中的最佳气动性能。随着迭代的进行,所输入的合适的目标层流区域长度参数逐步优化,最终收敛到一个对应优化跨音速自然层流翼型的参数。A suitable input generally refers to the best aerodynamic performance among a series of airfoils generated by parameter perturbation in this optimization step. As the iteration proceeds, the input parameters of the appropriate target laminar flow region length are gradually optimized, and finally converge to a parameter corresponding to the optimal transonic natural laminar flow airfoil.
本发明创造的有益效果:Beneficial effects created by the present invention:
本发明方法可使在飞机跨音速巡航飞行下,在(弱)激波-边界层的复杂流动环境中,实现翼型表面层流区域的扩大,从而延迟层流转捩的发生,实现摩擦阻力减小的目标。所获得的新的优良跨音速自然层流性能的翼型,可以应用于飞机机翼和发动机短舱剖面的设计优化之中。图5和图6分别展示了实验所获得的优化前后跨音速自然层流翼型表面层流区域长度增大的事实(其中高亮部分为层流区域,高亮部分和相对黑暗部分的分界线就是层流转捩地带)。攻角1°时,优化前初始翼型的层流区域长度69.2%单位弦长,优化后跨音速自然层流区域长度76.8%单位弦长;攻角4°时,优化前初始翼型的层流区域长度60.1%单位弦长,优化后跨音速自然层流区域长度63.5%单位弦长。The method of the invention can realize the enlargement of the laminar flow area on the surface of the airfoil in the complex flow environment of (weak) shock wave-boundary layer under the transonic cruising flight of the aircraft, thereby delaying the occurrence of laminar flow transition and realizing the reduction of frictional resistance small goals. The obtained new airfoil with excellent transonic natural laminar flow performance can be applied to the design optimization of aircraft wing and engine nacelle section. Figure 5 and Figure 6 respectively show the fact that the length of the laminar region on the surface of the transonic natural laminar flow airfoil before and after the optimization obtained by the experiment increases (the highlighted part is the laminar flow region, and the boundary between the bright part and the relatively dark part is the laminar transition zone). When the angle of attack is 1°, the length of the laminar flow region of the initial airfoil before optimization is 69.2% of the unit chord length, and the length of the transonic natural laminar flow region after optimization is 76.8% of the unit chord length; when the angle of attack is 4°, the layer of the initial airfoil before optimization The flow region length is 60.1% of the unit chord length, and the optimized transonic natural laminar flow region length is 63.5% of the unit chord length.
附图说明Description of drawings
图1为翼型表面流动中层流-湍流分布在优化前后的比较,说明了跨音速层流翼型设计意图。Figure 1 is a comparison of the laminar-turbulent flow distribution in the airfoil surface flow before and after optimization, illustrating the design intent of the transonic laminar flow airfoil.
图2为翼型流场计算时划分的流场网格示意。Figure 2 is a schematic diagram of the flow field mesh divided during the calculation of the airfoil flow field.
图3为基于人工神经网络的跨音速自然层流翼型设计优化方法示意。Fig. 3 is a schematic diagram of the design optimization method of transonic natural laminar flow airfoil based on artificial neural network.
图4为为了验证所用转捩模型的准确性的与风洞试验结果进行比较的图,说明了所用流场模拟求解器在判定层流区域长度上的可靠性。Figure 4 is a graph comparing the accuracy of the transition model used with the wind tunnel test results, illustrating the reliability of the flow field simulation solver used in determining the length of the laminar flow region.
图5为非跨音速自然层流翼型(上)与优化的跨音速自然层流翼型(下)在马赫数0.785来流下攻角1°的层流区域比较。Figure 5 is a comparison of the non-transonic natural laminar flow airfoil (upper) and the optimized transonic natural laminar flow airfoil (lower) at Mach number 0.785 in the laminar flow region with an angle of attack of 1°.
图6为非跨音速自然层流翼型(上)与优化的跨音速自然层流翼型(下)在马赫数0.785来流下攻角4°的层流区域比较。Figure 6 is a comparison of the non-transonic natural laminar flow airfoil (upper) and the optimized transonic natural laminar flow airfoil (lower) at a Mach number of 0.785 and a laminar flow region with an angle of attack of 4°.
图7为本发明优化设计流程图示。Fig. 7 is a flow chart diagram of the optimization design of the present invention.
具体实施方式Detailed ways
步骤(1):建立为了跨音速层流优化设计的翼型参数化方法。Step (1): Establish an airfoil parameterization method for optimal design of transonic laminar flow.
采用PARSEC参数化方法表达翼型外形,建立飞机翼型表达方式,参见表1。The PARSEC parameterization method is used to express the shape of the airfoil, and the expression method of the aircraft airfoil is established, see Table 1.
表1优化前某初始翼型几何参数Table 1 Geometric parameters of an initial airfoil before optimization
步骤(2)参数扰动,获得一系列翼型Step (2) parameter perturbation to obtain a series of airfoils
这里的优化过程为迭代过程的。在一次优化步骤中,首先,根据初始待优化翼型,分析得到对应的11个PARSEC几何参数;通过拉丁超立方采样技术(Owen,A.B.(1992)."Orthogonal arrays for computer experiments,integration and visualization".Statistica Sinica.2:439–452.)进行参数扰动,获得一系列的新的翼型对应几何参数。每次优化步骤中扰动的范围是逐渐减小的,以期最终收敛到一个优化了的跨音速层流翼型。针对通过参数扰动获得的一系列翼型,运用上面提到的流场计算方程进行流场计算并获得层流区域长度的结果。The optimization process here is an iterative process. In one optimization step, firstly, according to the initial airfoil to be optimized, the corresponding 11 PARSEC geometric parameters are analyzed; through the Latin hypercube sampling technique (Owen, A.B. (1992). "Orthogonal arrays for computer experiments, integration and visualization" .Statistica Sinica.2:439–452.) Perform parameter perturbation to obtain a series of new airfoil corresponding geometric parameters. The perturbation range is gradually reduced in each optimization step in order to eventually converge to an optimized transonic laminar airfoil. For a series of airfoils obtained by parameter perturbation, the flow field calculation equation mentioned above is used to calculate the flow field and obtain the result of the length of the laminar flow region.
在每一次优化步骤中,每个新翼型都有了对应的几何参数和层流区域长度的气动性能参数。本方法采用基于人工神经网络的代理模型建立两者的联系。在训练人工神经网络的时候,输入端为本次优化步骤的各个翼型的气动性能(层流长度),输出端为各个翼型的几何参数。然后进行训练获得代理模型。步骤(3):建立训练相关的人工神经网络。At each optimization step, each new airfoil has corresponding geometric parameters and aerodynamic performance parameters for the length of the laminar flow region. This method uses an agent model based on artificial neural network to establish the connection between the two. When training the artificial neural network, the input end is the aerodynamic performance (laminar flow length) of each airfoil in this optimization step, and the output end is the geometric parameters of each airfoil. Then perform training to obtain a proxy model. Step (3): Establish a training-related artificial neural network.
新翼型都有了对应的几何参数和层流区域长度的气动性能参数。采用代理模型进行两者的联系的建立。类似传统的反设计,在训练好的人工神经网络中输入一个合适的目标层流区域长度参数,以期获得对应新翼型的几何参数。该部分的设计优化思路参见图3。The new airfoils have corresponding geometric parameters and aerodynamic performance parameters for the length of the laminar flow region. The agency model is used to establish the connection between the two. Similar to the traditional inverse design, a suitable target laminar region length parameter is input into the trained artificial neural network in order to obtain the geometric parameters corresponding to the new airfoil. Refer to Figure 3 for the design optimization idea of this part.
随着优化步骤的迭代的进行,所输入的合适的目标层流区域长度参数逐步优化,最终收敛到一个对应优化跨音速自然层流翼型的参数。整个优化过程可以参见图7。图5和图6分别展示了实验所获得的优化前后跨音速自然层流翼型表面层流区域长度增大的事实(其中高亮部分为层流区域,高亮部分和相对黑暗部分的分界线就是层流转捩地带)。攻角1°时,优化前初始翼型的层流区域长度69.2%单位弦长,优化后跨音速自然层流区域长度76.8%单位弦长;攻角4°时,优化前初始翼型的层流区域长度60.1%单位弦长,优化后跨音速自然层流区域长度63.5%单位弦长。With the iteration of the optimization step, the input parameters of the appropriate target laminar flow region length are gradually optimized, and finally converge to a parameter corresponding to the optimal transonic natural laminar flow airfoil. The entire optimization process can be seen in Figure 7. Figure 5 and Figure 6 respectively show the fact that the length of the laminar region on the surface of the transonic natural laminar flow airfoil before and after the optimization obtained by the experiment increases (the highlighted part is the laminar flow region, and the boundary between the bright part and the relatively dark part is the laminar transition zone). When the angle of attack is 1°, the length of the laminar flow region of the initial airfoil before optimization is 69.2% of the unit chord length, and the length of the transonic natural laminar flow region after optimization is 76.8% of the unit chord length; when the angle of attack is 4°, the layer of the initial airfoil before optimization The flow region length is 60.1% of the unit chord length, and the optimized transonic natural laminar flow region length is 63.5% of the unit chord length.
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Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109484623A (en) * | 2018-11-07 | 2019-03-19 | 西北工业大学 | Wide speed domain lift line slope symmetrical airfoil design method and aerofoil profile |
| CN109933926A (en) * | 2019-03-19 | 2019-06-25 | 北京百度网讯科技有限公司 | Method and apparatus for predicting flight reliability |
| CN112084727A (en) * | 2020-10-26 | 2020-12-15 | 中国人民解放军国防科技大学 | A Transition Prediction Method Based on Neural Network |
| CN113111436A (en) * | 2021-04-15 | 2021-07-13 | 泉州装备制造研究所 | Airplane large component pre-connection layout and multi-constraint action sequence optimization method |
| CN113673031A (en) * | 2021-08-11 | 2021-11-19 | 中国科学院力学研究所 | A flexible airship service angle-of-attack identification method based on the fusion of strain response and deep learning |
| CN115688529A (en) * | 2022-11-14 | 2023-02-03 | 中航西安飞机工业集团股份有限公司 | Two-dimensional airfoil flow field grid generation method based on neural network proxy model |
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| CN119199360A (en) * | 2024-11-25 | 2024-12-27 | 四川航空股份有限公司 | Civil aviation fault monitoring method and system based on artificial intelligence |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7191161B1 (en) * | 2003-07-31 | 2007-03-13 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Method for constructing composite response surfaces by combining neural networks with polynominal interpolation or estimation techniques |
| CN103488847A (en) * | 2013-10-08 | 2014-01-01 | 北京航天长征飞行器研究所 | Aerodynamic shape optimization method based on neural network integration |
| CN104778327A (en) * | 2015-04-23 | 2015-07-15 | 复旦大学 | Airplane airfoil design optimization method based on artificial neural network |
| CN104834772A (en) * | 2015-04-22 | 2015-08-12 | 复旦大学 | Artificial-neural-network-based inverse design method for aircraft airfoils/wings |
| CN106547954A (en) * | 2016-10-17 | 2017-03-29 | 北京航空航天大学 | A kind of Airfoil Optimization method of the low reynolds number staggered floor wing |
-
2018
- 2018-05-17 CN CN201810472168.0A patent/CN108733914A/en active Pending
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7191161B1 (en) * | 2003-07-31 | 2007-03-13 | The United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration | Method for constructing composite response surfaces by combining neural networks with polynominal interpolation or estimation techniques |
| CN103488847A (en) * | 2013-10-08 | 2014-01-01 | 北京航天长征飞行器研究所 | Aerodynamic shape optimization method based on neural network integration |
| CN104834772A (en) * | 2015-04-22 | 2015-08-12 | 复旦大学 | Artificial-neural-network-based inverse design method for aircraft airfoils/wings |
| CN104778327A (en) * | 2015-04-23 | 2015-07-15 | 复旦大学 | Airplane airfoil design optimization method based on artificial neural network |
| CN106547954A (en) * | 2016-10-17 | 2017-03-29 | 北京航空航天大学 | A kind of Airfoil Optimization method of the low reynolds number staggered floor wing |
Non-Patent Citations (6)
| Title |
|---|
| F.R.MENTER等: "Transition Modelling for General Purpose CFD Codes", 《FLOW TURBULENCE COMBUST》 * |
| 孙燕杰等: "基于人工神经网络的机翼外形预测", 《力学季刊》 * |
| 李静: "高性能飞行器气动外形设计方法研究与应用", 《中国博士学位论文全文数据库工程科技Ⅱ辑》 * |
| 王一凡等: "考虑转捩点约束的自然层流翼型变弯度设计", 《航空计算技术》 * |
| 白俊强等: "超临界翼型稳健型优化设计研究", 《空气动力学学报》 * |
| 黄江涛等: "应用Delaunay图映射与FFD技术的层流翼型气动优化设计", 《航空学报》 * |
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|---|---|---|---|---|
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| CN112084727A (en) * | 2020-10-26 | 2020-12-15 | 中国人民解放军国防科技大学 | A Transition Prediction Method Based on Neural Network |
| CN113111436A (en) * | 2021-04-15 | 2021-07-13 | 泉州装备制造研究所 | Airplane large component pre-connection layout and multi-constraint action sequence optimization method |
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| CN113673031B (en) * | 2021-08-11 | 2024-04-12 | 中国科学院力学研究所 | Flexible airship service attack angle identification method integrating strain response and deep learning |
| CN115688529A (en) * | 2022-11-14 | 2023-02-03 | 中航西安飞机工业集团股份有限公司 | Two-dimensional airfoil flow field grid generation method based on neural network proxy model |
| CN115688529B (en) * | 2022-11-14 | 2025-06-17 | 中航西安飞机工业集团股份有限公司 | A method for generating mesh of two-dimensional airfoil flow field based on neural network proxy model |
| CN116451356A (en) * | 2023-05-23 | 2023-07-18 | 西安交通大学 | Uncertainty compatible natural laminar wing configuration gradient optimization design method |
| CN116451356B (en) * | 2023-05-23 | 2023-11-24 | 西安交通大学 | Uncertainty compatible natural laminar wing configuration gradient optimization design method |
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