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1.
纵向涡对近壁湍流影响的激光测试   总被引:3,自引:0,他引:3  
王家禄  张兆顺  单桦 《力学学报》1996,28(3):381-384
用激光测试方法详细地研究了单涡、上洗双涡、下洗双涡对近壁湍流的影响.在涡的下洗区,流体流速高,湍流度低,流体流向壁面;在涡的上洗区,流体流速低,湍流度高,流体远离壁面  相似文献   

2.
本文用快速涡方法对入射涡与圆柱的相互作用进行了数值模拟,观察到了入射涡在圆柱表面上诱导的二次分离和三次分离现象。二次涡的产生,与入射涡配对,改变了它们的运动轨迹。二次涡是入射涡“回跳”现象的主要原因。本文还对不同入射涡强度及相互位置作了计算,并分析了不同参数对涡运动轨迹的影响。这些现象与涡的无粘圆柱绕流有着本质的差异。  相似文献   

3.
以数值计算为手段,分析了带涡襟翼的翼型的流场特性,分别对迎角及扰流板偏角对翼型气动性能的影响做了分析。结果表明,在小迎角来流情况下,保持迎角不变,涡襟翼偏转角度越大,升力越小,阻力越大,呈现较好的线性关系。在大迎角情况下,绕翼型的流动发生分离,通过适当控制涡襟翼的偏转角度,能够有效的改善翼型的失速特性,从而达到流动控制的目的,迎角越大,涡襟翼所需偏转的角度越大。  相似文献   

4.
基于声涡转化对穿孔板切向流效应的研究   总被引:1,自引:0,他引:1  
建立了一种有关切向流对小孔声阻抗影响的小扰动势流模型,其要点是使用法向质点速度连续而非广为采用的质点位移连续边界条件来匹配小孔剪切层两侧的声场,并在小孔前缘施加 Kutta条件以反映切向流效应的机理——锐缘处的声涡转化;模型中还考虑了实际应用中经常遇到的小孔形状和穿孔板厚度两个重要因素.理论预测的声阻和声抗与实验结果吻合良好.  相似文献   

5.
剪切流动中声、涡弱非线性作用与声控流动机理   总被引:1,自引:0,他引:1  
对非均匀流(特别是平行剪切流)中声、涡运动模式的划分及其相互作用进行了弱非线性分析,着重研究了一阶声、涡作用产生二阶涡的情况,计算了二阶生成涡相对于一阶涡的时均放大倍数。从这一角度分析了声学控制流动问题,指出与声波发生作用的涡的性质以及涡频率与声频率之间的关系,并定性地讨论了声压阈值问题。  相似文献   

6.
分别用RANS-SA方法和DES方法对NACA0012翼端梢涡进行模拟计算,分析了梢涡区域网格局部加密对梢涡计算结果的影响,并与实验结果进行了对比.相比于RANS-SA方法,DES方法在梢涡流场计算中具有更好的适用性,能够得到更准确的流动信息和更精细的涡结构;另外,网格局部加密对脉动量的计算影响很大.通过对脉动量的分析发现,在近尾缘处,几股涡的融合产生了比较强烈的脉动,随着梢涡的逐渐稳定,脉动量也逐渐减小;现有的实验结果显示在偏下游处会产生梢涡的振荡现象,使统计脉动量增大,而本文计算中未发现该现象.  相似文献   

7.
纵向涡对近壁湍流结构的影响   总被引:1,自引:1,他引:1  
王家禄  张兆顺  曾兴 《力学学报》1994,26(5):625-630
在封闭水槽中用氢气泡方法观察了纵向涡对近壁湍流结构的影响,涡的下洗侧出现了展向距离较宽、流动较稳定的快斑区,流向速度快;涡的上洗侧出现了含有慢斑的区域,流动结构复杂,流向速度慢,纵向涡使下洗侧速度较快的流体流向壁面,使上洗侧速度较慢的流体远离壁面。  相似文献   

8.
波涡相互作用研究的某些进展(Ⅰ)   总被引:4,自引:1,他引:3  
吴介之 《力学进展》1991,21(4):430-443
波涡相互作用是当代非定常非线性流体力学的一个重要领域.本文评述了迄今人们对微扰纵波(声波,不包括激波)和横波(涡波)与层状和轴状涡相互作用的研究进展,包括涡声理论、锐缘及光滑表面涡层分离以及自由涡层的2维感受性和非定常Kutta条件,波产生时均涡流的非线性Eulcr整流和广义Lagrange整流,波涡共振等课题的进展.还介绍了用非定常激发实施涡控制这一重要应用领域的一些新进展.   相似文献   

9.
大涡模拟的壁模型及其应用   总被引:3,自引:0,他引:3  
大涡模拟是研究湍流的非定常特性的重要方法. 但解析壁面层的大涡模拟所需的计算量与直接数值模拟相当,是大涡模拟在高雷诺数壁湍流数值模拟中所面临的主要困难. 解析壁面层所需的网格尺度与壁面黏性长度同量级,是引起壁湍流大涡模拟计算量增加的主要原因. 壁模型通过模化近壁流动避免了完全解析壁面层,可以显著地降低壁湍流大涡模拟的计算量,是克服上述困难的有效方法. 本文介绍了大涡模拟壁模型的主要类型;详细讨论了常用的壁面应力模型,特别是平衡层模型和双层模型的构建思路和特点;基于近壁流动的特征讨论了应力边界条件的必要性和适用性;指出了壁面应力模型的局限性以及考虑非平衡效应修正的各种方法;讨论了壁面应力模型的研究历史、最新进展和发展趋势,给出了常用的壁面应力模型的分支与发展关系图;并基于Werner-Wengle模型实现了周期山状流的大涡模拟.   相似文献   

10.
N表面张力对近固壁二空化泡影响的数值研究   总被引:1,自引:0,他引:1  
在忽略浮力下,用边界积分方法数值模拟了表面张力对固壁之上且靠近固壁的二轴对称空化泡生长和溃灭的影响,发现在下空泡最大等效半径为上空泡一半情形,若固壁对下空泡的Bjerknes力大于上空泡对下空泡的Bjerknes力,则表面张力的作用将使下空泡溃灭加速,使其向下的液体射流变强变宽;若固壁对下空泡的Bjerknes力小于上空泡对下空泡的Bjerknes力,则表面张力的作用将使下空泡溃灭变慢,使其向上射流变弱变细长;若这两个Bjerknes力近于相等,则表面张力将会对下空泡溃灭有重大作用,如改变下空泡射流的方向甚至形式(如由环状变向下或由向上变环状),当上空泡等于或小于下空泡时,表面张力将不会对这两个空泡的行为产生显著影响,定性地分析了表面张力作用的机理。  相似文献   

11.
A numerical solution of the equations of motion and energy supplemented with a differential turbulence model is obtained for the boundary layer on a wall in a compressible flow. Two approaches to determining the temperature of a thermally-insulated permeable wall are considered. The dependence of the temperature recovery coefficient on the permeability parameter approximating the calculated results is derived and compared with experimental data.  相似文献   

12.
13.
The interaction between the wake of a transverse circular cylinder and the underlying flat-plate boundary layer with a moderate gap ratio G/D=1.0 is investigated using both hydrogen-bubble-based and PIV-based visualization techniques. The spanwise rollers in the cylinder wake are found to be capable of inducing secondary vortices in the near-wall region. The mutual induction from the counter-clockwise rollers, which are closer to the wall, plays a primary role, so that these secondary vortices present linear lift-up motion at first. Their subsequent evolution dominantly determines the characteristics of the wake/boundary-layer interaction. Two different vortex interaction scenarios are observed: the secondary vortices can be either entrained into the rollers or pushed down towards the wall. This leads to a rapid three-dimensional destabilization process, through which streamwise vortices are generated. And it is suggested that these streamwise vortices are the dominant structures to promote the following boundary layer transition.  相似文献   

14.
In the present work, large eddy simulations of the flow field around a NACA-0012 aerofoil near stall conditions are performed at a Reynolds number of 5 × 104, Mach number of 0.4, and at various angles of attack. The results show the following: at relatively low angles of attack, the bubble is present and intact; at moderate angles of attack, the laminar separation bubble bursts and generates a global low-frequency flow oscillation; and at relatively high angles of attack, the laminar separation bubble becomes an open bubble that leads the aerofoil into a full stall. Time histories of the aerodynamic coefficients showed that the low-frequency oscillation phenomenon and its associated physics are indeed captured in the simulations. The aerodynamic coefficients compared to previous and recent experimental data with acceptable accuracy. Spectral analysis identified a dominant low-frequency mode featuring the periodic separation and reattachment of the flow field. At angles of attack α ≤ 9.3°, the low-frequency mode featured bubble shedding rather than bubble bursting and reformation. The underlying mechanism behind the quasi-periodic self-sustained low-frequency flow oscillation is discussed in detail.  相似文献   

15.
Shock formation due to flow compressibility and its interaction with boundary layers has adverse effects on aerodynamic characteristics, such as drag increase and flow separation. The objective of this paper is to appraise the prac-ticability of weakening shock waves and, hence, reducing the wave drag in transonic flight regime using a two-dimensional jagged wall and thereby to gain an appropriate jagged wall shape for future empirical study. Different shapes of the jagged wall, including rectangular, circular, and triangular shapes, were employed. The numerical method was validated by experimental and numerical studies involving transonic flow over the NACA0012 airfoil, and the results presented here closely match previous experimental and numerical results. The impact of parameters, including shape and the length-to-spacing ratio of a jagged wall, was studied on aerodynamic forces and flow field. The results revealed that applying a jagged wall method on the upper surface of an airfoil changes the shock structure significantly and disinte-grates it, which in turn leads to a decrease in wave drag. It was also found that the maximum drag coefficient decrease of around 17%occurs with a triangular shape, while the max-imum increase in aerodynamic efficiency (lift-to-drag ratio) of around 10%happens with a rectangular shape at an angle of attack of 2.26?.  相似文献   

16.
The flow over a flat plate delta wing at incidence and in sideslip is studied using vortex lattice models based on streamwise penelling. For the attached flow problem the effect of sideslip is simulated by modifying the standard vortex lattice model for zero sideslip by aligning the trailing vortices aft of the wing along the resultant flow direction. For the separated flow problem a non-linear vortex lattice model is developed for both zero and non-zero sideslip angles in which the shape and position of the leading edge separation vortices are calculated by an iterative procedure starting from an assumed initial shape. The theoretical values are compared with available theoretical and experimental results.  相似文献   

17.
基于势流理论建立水下爆炸气泡运动三维模型,采用边界积分法求解拉普拉斯方程,得到气泡的变形及位置,并在计算过程中引入弹性网格技术,避免了因网格扭曲而导致的数值发散,进而模拟了刚性壁面附近三维气泡的动态特性。在数值模拟过程中,将本文计算值与实验数据进行对比分析,结果表明,计算值与实验数据吻合良好。在此基础上,分别模拟了弱浮力、强Bjerknes力,强浮力、弱Bjerknes力以及浮力与Bjerknes力相当时壁面附近气泡的运动特征,并将各种工况的计算结果与基于开尔文冲量理论(Kelvin Impulse)的Blake准则进行对比分析与讨论,得到了不同参数下气泡的运动特征。  相似文献   

18.
Two techniques that improve the aerodynamic performance of wind turbine airfoils are described. The airfoil S809, designed specially for wind turbine blades, and the airfoil FX60-100, having a higher lift-drag ratio, are selected to verify the flow control techniques. The flow deflector, fixed at the leading edge, is employed to control the boundary layer separation on the airfoil at a high angle of attack. The multi-island genetic algorithm is used to optimize the parameters of the flow deflector. The results indicate that the flow deflector can suppress the flow separation, delay the stall, and enhance the lift. The characteristics of the blade tip vortex, the wake vortex, and the surface pressure distributions of the blades are analyzed. The vortex diffuser, set up at the blade tip, is employed to control the blade tip vortex. The results show that the vortex diffuser can increase the total pressure coefficient of the core of the vortex, decrease the strength of the blade tip vortex, lower the noise, and improve the efficiency of the blade.  相似文献   

19.
对槽道内涡波流场的瞬态速度矢量场进行了2DPIV测量实验,将2DPIV测量的矢量场数据进行POD分析,根据POD分解的各阶模态的能量比确定了表征涡波流场主导结构的前15阶模态。结果表明,POD分解的前15阶模态发现槽道内涡波流场是由槽道壁面剪切层诱导的涡列以及伴随的波状主流组成;流场中大尺度的涡旋发展为涡对,对波状主流的脉动频率产生影响;根据涡波流场中的驻点和鞍点,获取了流场的大尺度涡对、平均流场以及Helmholtz涡环等明显特征;最后根据POD分解的前15阶模态对槽道内涡波流场进行重组,重组流场表征了槽道内层流状态下波状主流的形态和涡旋共存的涡波结构以及驻点和鞍点的位置处涡旋的变化等主要特征,有效地剔除了PIV测量流场中的随机信息,保留了PIV测量流场的主导特征。  相似文献   

20.
针对阶梯圆柱形耦合声场建模问题,提出基于特征正交-里兹能量原理的声学建模方法.该方法利用二维特征正交多项式和周向傅里叶级数表征阶梯圆柱形耦合声场子分段的声压函数,从能量角度考虑邻近子声场间声学连续性条件,并结合里兹法获得耦合声场的声学特性.基于本建模方法对不同分段的耦合声场开展声学特性分析,结果表明,本建模方法在保证计算准确性的基础上有效提高了计算效率,且对任意阶梯分段的圆柱形耦合声场普遍适用;圆柱形耦合声场固有频率会随着腔体外径增大而普遍增大,而腔深的影响规律相反;降低声学边界阻抗可抑制声学响应幅值,为此类声场的噪声控制提供了设计依据.  相似文献   

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