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1.
用热线风速仪研究多段翼型前缘缝翼在不同条件下流动速度的定常性和非定常性。结合多段翼型定常流动Navier-Stokes方程数值模拟的结果,分析了迎角、后缘襟翼参数(偏角、缝道宽度、搭接量)对缝翼定常和非定常流动速度的影响规律。研究结果表明:在缝翼后缘处,流动分为缝道加速流动区、缝翼尾流区、缝翼上表面以上的主流区;缝翼尾流区流动速度非定常性主要表现在中低频率范围(2k Hz以下),而缝道加速流动区和缝翼上表面以上的主流区流动非定常性常表现出高频特性(2k Hz以上);在失速前随迎角增加,或者当襟翼偏角从20°向30°增加时,缝道流动加速,槽区涡减小;缝翼槽区涡形成和振荡是中低频率范围流动非定常性的机理,而缝翼鼻尖脱落涡是缝翼槽区涡振荡的激励因素。  相似文献   

2.
基于kω的SST两方程湍流模型,在时间域求解雷诺平均Navier-Stokes方程,模拟弯度翼型大迎角时的分离流动。通过给翼型施加一定形式的扰动,重点关注了翼型弯度对大迎角分离涡流场平衡态转移的影响。研究结果表明:与相同厚度20%以上的对称翼型相比,2%弯度的翼型出现分离涡流场平衡态转移的起始迎角变小2°左右,迎角区间变宽约1°;在厚度相对较小的NACA2416翼型上也发现上述分离涡平衡态转移现象。由此说明翼型弯度在一定程度上促使了分离涡平衡态的转移。  相似文献   

3.
为进一步提高倾转旋翼机悬停状态下的有效载重,开展了定常吹气流动控制对向下载荷的影响研究。首先应用延迟脱体涡模拟(DDES)方法对翼型-90°迎角下非定常大范围分离流动结构进行了数值分析;然后分别开展了前缘吹气、后缘吹气降载措施研究,揭示了吹气降载的机理,并对不同吹气口位置和吹气动量系数的影响进行了定量分析,最后开展了前、后缘同时吹气作用下降载数值模拟研究。计算结果表明:前缘最佳吹气位置在翼型的前缘点,而后缘吹气最佳位置位于襟翼弦长的15%处;前缘吹气的降载效果要优于后缘吹气,而且吹气动量系数对向下载荷的影响较小;相对于初始未施加流动控制构型,阻力系数减小量可达到32.72%。  相似文献   

4.
三角翼的双襟翼控涡作用的数值模拟研究   总被引:2,自引:0,他引:2  
袁礼  忻鼎定 《力学学报》2000,32(2):151-158
对装有“前端襟翼”和“前缘襟翼”的74°后掠三角翼的不可压缩流场作了数值模拟,以研究襟翼的旋涡控制作用.数值模拟是用拟压缩性方法求解一般曲线坐标系下的三维不可压缩Navier-Stokes方程,时间离散用向后Euler差分,空间无粘项的离散用二阶迎风TVD格式,所得的离散方程用对角化形式的近似隐式因子分解格式求解.湍流模型用Baldwin-Lomax代数模式.计算了三种平面形状的机翼在迎角范围为10°~50°的绕流和气动特性.计算和实验的比较表明,襟翼向下偏转可以推迟旋涡破裂,且对提高机翼的减阻能力、升阻比和改善失速前后的气动特性有明显效果,双襟翼具有更佳的控涡效果.  相似文献   

5.
针对直升机旋翼反流区因反流动态失速导致的非定常载荷、阻力激增以及负升力等问题,开展了基于后缘小翼的翼型反流动态失速主动控制试验研究.采用动态压力测量结合翼型表面压力积分的方法,重点分析了后缘小翼不同的振荡相位差、幅值和减缩频率对反流动态失速控制的影响规律,对比了后缘小翼动态偏转和固定偏转的差异,试验雷诺数Re=3.5×105.结果表明,当后缘小翼与翼型以相同的频率正弦振荡运动,且二者的相位差为0°时,能改善反流动态失速过程中钝几何前缘的流动分离,并在反流状态下实现了翼型负升力系数下降21.2%,阻力系数下降37.5%,俯仰力矩系数迟滞环面积下降44.6%的控制效果;动态偏转的后缘小翼对翼型反流动态失速的控制效果随后缘小翼振荡幅值的增加而增加,但进一步增加振荡幅值对于控制效果的提升有限;当减缩频率增加时,动态偏转的后缘小翼对反流状态下翼型阻力的控制效果会更加明显;后缘小翼的动态偏转与固定偏转都能有效改善翼型在反流中的动态气动性能,但是动态偏转对于不同翼型迎角的适应能力优于固定偏转,并取得了更好的非定常载荷控制以及更好的阻力和负升力改善效果.  相似文献   

6.
基于$k$-$\omega$的SST两方程湍流模型, 求解雷诺平均N-S方程获得定常和非定常气动力, 耦合 翼型弹性振动方程, 在时间域内模拟了不同的翼型非定常流动, 重点研究了大迎角下的分离 流问题, 研究结果表明: 在百万雷诺数条件下, 由于振动引起分离涡的不规律脱落, 可能导 致气动力平均值的变化; 而厚度大于20\%的翼型在一定大迎角范围内, 会出现分离涡流场平 衡态的转化, 从流体力学稳定性的角度, 解释了风洞实验中大迎角气动力数据的分散性, 为 大迎角气动力风洞实验的重复性和数据分散性给出了一种新解释.  相似文献   

7.
低Reynolds数NACA0012翼型绕流的流动特性分析   总被引:1,自引:0,他引:1  
吴鋆  李天  王晋军 《实验力学》2014,29(3):265-272
在水槽中应用PIV测速技术研究了NACA0012翼型在Reynolds数为8200时的流动特性,重点关注了翼型绕流结构中主频和扰动增长速率随迎角的变化。结果表明,分离剪切层的扰动增长符合指数规律;且随着迎角的增大,转捩过程加速,表现为扰动增长率逐渐增大,转捩的起始位置逐渐向上游移动。在所有实验迎角情况下,流场均由脱落旋涡主导,但其主导作用随着迎角的增大而削弱。  相似文献   

8.
王良益 《实验力学》1993,8(1):70-75
本文采用水洞流谱观测方法,研究了带有涡襟翼的翼—身组合体前缘分离涡及涡系干扰的流动特性,并与普通翼—身组合体情况进行比较;分析了涡襟翼的涡流运动特点及其升阻比增大的机理;讨论了翼—身组合体涡系干扰的主要反映及对涡破碎特性的影响;并对非对称体涡出现的条件以及分离旋涡在稳定发展过程中的抗干扰能力提出了看法.  相似文献   

9.
结合基于$k$-$\omega$的SST两方程湍流模型,求解雷诺平 均Navier-Stokes方程获得定常和非定常气动力,耦合翼型弹性运动方程,在时间 域内模拟了不同厚度对称翼型在不同迎角下的气动弹性动态过程, 并重点研究了较大迎角下的不同厚度翼型流场特征和气动弹性的性质,研究结果表明:在论 文所涉及的参数情况下,对于迎角从零到大迎角范围,翼型颤振临界速度随迎角的变化不是 单调的. 翼型颤振临界速度迅速下降的起始迎角比最大升力系数对应的迎角小很多.  相似文献   

10.
使用雷诺平均NS方程、采用Johnson-King紊流模型、嵌套网格和有限体积法研究大迎角下的多缝道的多段翼型绕流。利用嵌合体技术对组合每一部分生成高质量并适于高效求解的贴体网格;将J-K模型发展应用于计算缝道流动以及具有边界层、尾迹流交汇的复杂流动。以具有17%相对厚度的GAW-1翼型带30%襟翼翼型及一个三段翼型为例进行了计算,计算结果与实验结果吻合很好,证实该方法可以较好地预示多段翼型上的粘性绕流、多缝道流动与最大升力。  相似文献   

11.
The possibility of controlling the aerodynamic characteristics of airfoils in transonic flight regimes by means of one-sided pulsed-periodic energy supply is studied. Based on the numerical solution of two-dimensional unsteady gas-dynamic equations, the change in the flow structure in the vicinity of a symmetric airfoil at different angles of attack and the aerodynamic characteristics of the airfoil as functions of the amount of energy supplied asymmetrically (with respect to the airfoil) are determined. The results obtained are compared with the data calculated for the flow past the airfoil at different angles of attack without energy supply. It is found that a given lift force can be obtained with the use of energy supply at a much better lift-to-drag ratio of the airfoil, as compared to the case of the flow past the airfoil at an angle of attack. The moment characteristics of the airfoil are found. __________ Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 49, No. 6, pp. 82–87, November–December, 2008.  相似文献   

12.
In this research, the effect of flow regime change from subsonic to transonic on the air loads of a pitching NACA0012 airfoil is investigated. To do this, the effect of change in flow regime on the lift and pitching moment coefficients hysteresis cycles is studied. The harmonic balance approach is utilized for numerical calculation due to its low computational time. Verifications are also made with previous works and good agreements are observed. The assessment of flow regime change on the aforementioned hysteresis cycles is accomplished in the Mach number range of M=0.65–0.755. The reduced frequency and pitch amplitude also vary from k=0.03 to 0.1 and α0=1–2.51°, respectively. Results show that the effect of increase in Mach number is to increase and decrease the lift coefficient during downstroke and upstroke, respectively, whereas at low reduced frequencies, the effect of increase in Mach number may lead to a reverse manner when airfoil moves toward its extremum angle of attack. Results also reveal that as the pitch amplitude varies, the shape of lift coefficient hysteresis cycle depends more on the pitch amplitude than on the appearance of shock. It is shown that as the Mach number increases, the incidence angles correspond to the extremum pitching moment, and depending on the reduced frequency, lie between zero and extremum angle of attack. These incidence angles shift toward the extremum angle of attack as the reduced frequency decreases. Results also show that the increase in pitch amplitude at low Mach number, in such a way that leads to the formation of shock around the extremum angle of attack, causes the extremum pitching moment to appear around these angles and at high Mach number, depending on the reduced frequency, the extremum pitching moment incidence angles would be between zero and extremum incidence angle.  相似文献   

13.
Flow past multi-element airfoil is studied via two-dimensional numerical simulations. The incompressible Reynolds averaged Navier–Stokes equations, in primitive variables, are solved using a stabilized finite element formulation. The Spalart–Allmaras and Baldwin–Lomax models are employed for turbulence closure. The implementation of the Spalart–Allmaras model is verified by computing flow over a flat plate with a specified trip location. Good agreement is seen between the results obtained with the two models for flow past a NACA 0012 airfoil at 5° angle of attack. Results for the multi-element airfoil, with the two turbulence models, are compared with experiments for various angles of attack. In general, the pressure distribution, from both the models matches quite well with the experimental results. However, at larger angles of attack, the computational results overpredict the suction peak on the slat. The velocity profiles from the Baldwin–Lomax model are, in general, more diffused compared to those from the Spalart–Allmaras model. The agreement between the computed and experimental results is not too good in the flap region for large angles of attack. Both the models are unable to predict the stall; the flow remains attached even for relatively large angles of attack. Consequently, the lift coefficient is over predicted at large α by the computations. Overall, compared to the Baldwin–Lomax model, the predictions from the Spalart–Allmaras model are closer to experimental measurements.  相似文献   

14.
平板大攻角绕流升力和阻力系数的计算   总被引:1,自引:0,他引:1  
二维平板或二维对称薄翼型大攻角绕流升力和阻力系数与攻角之间存在的函数关系一般用数据表格的形式给出。本文根据垂直平板绕流阻力实验数据和对称薄翼型全攻角绕流实验数据,分析得到了平板大攻角绕流总压力及其升力分量和阻力分量系数的近似计算公式。结果表明:平板总压力系数约等于攻角正弦值的2倍;总压力的阻力分量系数约等于攻角正弦值平方的2倍;升力分量系数约为攻角2倍的正弦值。计算结果与两组试验数据具有较好的一致性。  相似文献   

15.
The possibility of controlling the aerodynamic characteristics of airfoils in transonic flight regimes by means of local pulsed periodic energy supply is considered. The numerical solution of two-dimensional unsteady equations of gas dynamics allowed determining the changes in the flow structure near a symmetric airfoil and its aerodynamic characteristics depending on the magnitude of energy in the case of its asymmetric (with respect to the airfoil) supply. The results obtained are compared with the calculated data for the flow around the airfoil at different angles of attack without energy supply. With the use of energy supply, a prescribed lift force can be obtained with a substantially lower wave drag of the airfoil, as compared with the flow around the airfoil at an angle of attack. __________ Translated from Prikladnaya Mekhanika i Tekhnicheskaya Fizika, Vol. 48, No. 6, pp. 70–76, November–December, 2007.  相似文献   

16.
A. I. Ruban 《Fluid Dynamics》1982,17(6):860-867
Numerous experiments on subsonic flow of gas past thin wing profiles (see the reviews [1, 2]) have shown that the flow near the leading edge of an airfoil is separationless only at angles of attack less than a certain critical value, which depends on the shape of the airfoil. If the angle of attack reaches the critical value, a closed region of recirculation flow of small extension is formed on the upper surface of the airfoil. Under ordinary flow conditions, the boundary layer on the leading edge of the airfoil remains laminar in the entire preseparation range of angles of attack. However, the appearance of the closed separation region is, as a rule, accompanied by transition from a laminar to a turbulent flow regime. Moreover, generation of turbulence is observed precisely in the flow separation region. The present paper is devoted to a study of the stability of the boundary layer on the leading edge of a thin airfoil in a flow of incompressible fluid. The case when the angle of attack of the airfoil relative to the oncoming flow differs little from the critical value is considered.Translated from Izvestiya Akademii Nauk SSSR, Mekhanika Zhidkosti i Gaza, No. 6, pp. 55–63, November–December, 1982.  相似文献   

17.
Bio-inspired corrugated airfoils show favourable aerodynamic characteristics such as high coefficient of lift and delayed stall at low Reynolds numbers. Two-dimensional (2D) direct numerical simulation has been performed here on a corrugated airfoil at various angles of attack (0°, +5°, -5°) and Reynolds number of 280 to 6700. The objective is to analyse the pressure variation inside the corrugations and correlate it to the vortex movement across the corrugations and the overall aerodynamic characteristics of the corrugated airfoil. The flow characteristics have been examined based on the local Strouhal numbers in the corrugations of the airfoil. It is observed that the pressure variation in each corrugation is the result of vortex merging and separation in the corrugation which plays a major role in changing the flow characteristics. The Strouhal number of the flow is dictated by the most dominant local Strouhal number. The numerical results are further compared with experimental results obtained using particle image velocimetry, and the two set of results are found to match well. These results are significant because they elucidate the effect of corrugation, angle of attack, and Reynolds number on flow over a corrugated airfoil.  相似文献   

18.
Micro Air Vehicles (MAVs) can be difficult to control in the outdoor environment as they fly at relatively low speeds and are of low mass, yet exposed to high levels of freestream turbulence present within the Atmospheric Boundary Layer. In order to examine transient flow phenomena, two turbulence conditions of nominally the same longitudinal integral length scale (Lxx/c?=?1) but with significantly different intensities (Ti?=?7.2?% and 12.3?%) were generated within a wind tunnel; time-varying surface pressure measurements, smoke flow visualization, and wake velocity measurements were made on a thin flat plate airfoil. Rapid changes in oncoming flow pitch angle resulted in the shear layer to separate from the leading edge of the airfoil even at lower geometric angles of attack. At higher geometric angles of attack, massive flow separation occurred at the leading edge followed by enhanced roll up of the shear layer. This lead to the formation of large Leading Edge Vortices (LEVs) that advected at a rate much lower than the mean flow speed while imparting high pressure fluctuations over the airfoil. The rate of LEV formation was dependent on the angle of attack until 10° and it was independent of the turbulence properties tested. The fluctuations in surface pressures and consequently aerodynamic loads were considerably limited on the airfoil bottom surface due to the favorable pressure gradient.  相似文献   

19.
Airfoil self-noise is a common phenomenon for many engineering applications. Aiming to study the underlying mechanism of airfoil self-noise at low Mach number and moderate Reynolds number flow, a numerical investigation is presented on noise generation by flow past NACA0018 airfoil. Based on a high-order accurate numerical method, both the near-field hydrodynamics and the far-field acoustics are computed simultaneously by performing direct numerical simulation. The mean flow properties agree well with the experimental measurements. The characteristics of aerodynamic noise are investigated at various angles of attack. The obtained results show that inclining the airfoil could enlarge turbulent intensity and produce larger scale of vortices. The sound radiation is mainly towards the upper and lower directions of the airfoil surface. At higher angle of attack, the tonal noise tends to disappear and the noise spectrum displays broad-band features.  相似文献   

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