共查询到20条相似文献,搜索用时 15 毫秒
1.
I. I. Vigdorovich 《Journal of Experimental and Theoretical Physics》2005,101(4):741-759
A complete theory of turbulent boundary layer flow over a flat plate with uniform wall suction is proposed. The theory relies on an asymptotic analysis of the Reynolds equations and dimensional considerations and does not involve any special closure hypotheses. Characteristics of the turbulent boundary layer with suction are calculated for the entire range of flow parameters by using the known characteristics of a reference flow (turbulent boundary layer over an impermeable flat plate). The velocity and shear stress profiles, the distribution of skin friction along the plate, and integral flow characteristics are obtained by using only the known velocity profile in the reference flow. The normal Reynolds stresses are calculated by using analogous characteristics of the reference flow. Results are presented in terms of scaling variables. 相似文献
2.
V. I. Kornilov 《Thermophysics and Aeromechanics》2010,17(2):249-258
Experiments are performed to study the possibility of decreasing the net drag of a flat plate with the use of streamwise-oriented
vertical elements mounted normal to the surface in an incompressible equilibrium turbulent boundary layer. The Reynolds number
based on the boundary-layer momentum thickness in the section where the vertical elements are placed is 820. It is demonstrated
that vertical large eddy breakup elements with the geometry used do not reduce the drag of a flat plate in the major part
of the range of Reynolds numbers Re
x
examined. It is only at extremely low values of Re
x
that a certain gain in the net drag is reached, as compared with the value for a non-modified flow. 相似文献
3.
Experimental modeling of air blowing into a turbulent boundary layer using an external pressure flow
We have experimentally investigated the characteristics of an incompressible turbulent boundary layer on a plane plate upon the passive blowing of air through a fine-perforated surface and flushing it by supplying an external pressure flow through a wind tunnel using an intake device equipped with an attachment for draining the boundary layer on the inactive side of the plate. A stable decrease in the local values of the surface coefficient of friction, which reaches 80% at the end of the perforated region, has been detected over the length of the plate. The possibility of controlling surface friction by changing the velocity of the external flow and selecting the meshes and filters at the inlet to the flow passage has been demonstrated. 相似文献
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A. V. Smol’yakov 《Acoustical Physics》2010,56(6):1080-1088
A theory is constructed that makes it possible to calculate the initial parameters necessary for calculating the hydrodynamic
(turbulent) noise, which is a handicap to the operation of sea geophysical antennas. Algorithms are created for calculating
the profile and defect of the average speed, displacement thickness, momentum thickness, and friction resistance in a turbulent
boundary layer on a cylinder in its axial flow. Results of calculations using the developed theory are compared to experimental
data. As the diameter of the cylinder tends to infinity, all relations of the theory pass to known relations for the boundary
layer on a flat plate. The developed theory represents the initial stage of creating a method to calculate hydrodynamic noise,
which is handicap to the operation of sea geophysical antennas. 相似文献
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Simulation of a thick turbulent boundary layer via a rod grid 总被引:1,自引:0,他引:1
A possibility to simulate a thick Clauser-equilibrium incompressible turbulent boundary layer on a flat plate of finite length with the help of a grid formed by cylindrical rods was experimentally examined. A grid with rods oriented parallel to the streamlined surface proved to be an efficient tool enabling modification of the turbulent boundary layer. In most cases, at a distance of 600 rod diameters the time-average and fluctuation characteristics of the modified boundary layer exhibited values typical of a natural turbulent boundary layer. It is shown that the mean velocity profiles with artificially increased boundary-layer thickness can be represented, to a good accuracy, in terms of law-of-the-wall variables, and they can be generalized with a single dependence using an empirical velocity scale in the outside region. The use of a combined method for exerting an influence on the shear flow capable of improving the modeling procedure for turbulent velocity fluctuations in boundary layer is proposed. 相似文献
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A series of direct numerical simulations of the flow past a flat plate with two and eight rows of dimples in a staggered arrangement is carried out. The Reynolds number based on the boundary layer thickness and freestream velocity near the inflow plane is 1000 and the dimples are spherical with a depth to diameter ratio of 0.1. The incoming flow is laminar and the boundary layer thickness before the dimples is half the dimple depth. At this low Reynolds number the flow is expected to remain laminar over a smooth flat plate. The presence of the dimples triggers instabilities that cause significant momentum transport. It is shown that the shear layer that forms as the flow separates over the first two rows of dimple becomes unstable and sheds coherent vortex sheets. The vortex sheets become unstable and are transformed into packets of horseshoe vortices. When these vortices evolve over a flat plate or over a series of dimples the flow dynamics are very different with important changes in momentum transport across the boundary layer. 相似文献
11.
Farzin Ghanadi Maziar Arjomandi Benjamin S. Cazzolato Anthony C. Zander 《Journal of Turbulence》2013,14(8):705-728
This study investigates the changes in the structure of a turbulent boundary layer downstream of a flow-excited Helmholtz resonator. To this end, a fully developed turbulent boundary layer over a resonator mounted flush with a flat plate was simulated by implementing a large eddy simulation (LES). To assist in understanding the effect of the resonator on the flow structure, a sensitivity study was undertaken by changing the main geometrical parameters of the resonator. The results demonstrated that when the boundary layer thickness equals the orifice length, the cross-stream component of velocity fluctuations penetrates the boundary layer, resulting in a reduction of the turbulence intensity by up to 12%. Therefore, it is concluded that a Helmholtz resonator has the potential to reduce the instabilities within the boundary layer. These investigations also assist in identifying the optimal parameters to delay turbulence events within the grazing flow using Helmholtz resonators. 相似文献
12.
本文在高超声速脉冲式风洞内对基于纳米示踪的平面激光散射技术(nano-based planar laser scattering, NPLS)的应用进行了探索, 并在此基础上对平板边界层流动结构的精细测量进行了研究. 试验来流Ma=7.3, 总压4.8 MPa, 总温680 K. 通过时序的分析和调试, 对各分系统实现了高精度的同步控制; 定量的粒子注入及混合, 实现了粒子的均匀撒播, 对主流获得了均匀的显示效果; 对于边界层流动, 获得了精细的瞬态流动结构图像, 显示了层流到湍流的转捩过程, 并分析了其时空演化特性. 相似文献
13.
Formation of the turbulent boundary layer at air blowing through a wall with an abrupt change in boundary conditions 总被引:1,自引:0,他引:1
Development of an incompressible turbulent boundary layer with air blowing through a finely perforated flat surface, consisting of a permeable region and impermeable region behind, was studied experimentally. The mass flow rate of injected air Q per an area unit was varied from 0 to 0.2 (kg/s)/m2. Detailed data about the internal structure of the boundary layer in the flow region, characterized by an abrupt change in the flow conditions at the boundary of permeable and impermeable regions, were obtained. A consistent decrease in the local values of skin friction coefficient along a permeable sample and with an increase in the values of Q, reaching 90% at maximal Q, is shown. The role of the flow region behind the zone with an abrupt change in the boundary conditions, essential from the viewpoint of skin friction reduction, is revealed. 相似文献
14.
Direct numerical simulation of the turbulent boundary layer over a sharp cone with 20° cone angle (or 10° half-cone angle)
is performed by using the mixed seventh-order up-wind biased finite difference scheme and sixth-order central difference scheme.
The free stream Mach number is 0.7 and free stream unit Reynolds number is 250000/inch. The characteristics of transition
and turbulence of the sharp cone boundary layer are compared with those of the flat plate boundary layer. Statistics of fully
developed turbulent flow agree well with the experimental and theoretical data for the turbulent flat-plate boundary layer
flow. The near wall streak-like structure is shown and the average space between streaks (normalized by the local wall unit)
keeps approximately invariable at different streamwise locations. The turbulent energy equation in the cylindrical coordinate
is given and turbulent energy budget is studied. The computed results show that the effect of circumferential curvature on
turbulence characteristics is not obvious. 相似文献
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Based on fine measurement of time-averaged data of hot-wire anemometer we have developed the method determining local values
of skin-friction coefficient in the vicinity of the wall on the planar porous surface at the flow past which the noncanonical
turbulent boundary layer is formed. The method may be applied at investigation of the efficiency of various effects on the
incompressible boundary layer, in particular, with microblowing of air where usage of direct methods of friction determination
is complicated. 相似文献
17.
The turbulent boundary layer that forms downstream of a surface discontinuity is locally inhomogeneous. Here, we consider the boundary layer that occurs downstream of a rearward facing step discontinuity on a flat plate that is exposed to a zero incidence, uniform subsonic flow. The wall pressure "point" spectra are measured by small, flush-mounted pressure transducers located at various locations downstream of the step. A new form of the non-dimensional point wall pressure auto-frequency spectrum is proposed that includes the statistical variations of the reattachment location. This form is shown to collapse quite well all of the spectra measured slightly upstream, within, and downstream of the flow reattachment location. 相似文献
18.
Abstract
Evolution of the Λ-vortex and its transformation into the turbulent spot in a flat plate boundary layer are investigated experimentally. Extensive measurements visualizing the Λ-structure transformation into the turbulent spot on the smooth and ribbed surfaces of the flat plate are presented. The flow behavior in the course of spatial evolution of the Λ-structure and turbulent spot is discussed. Specific features of the downstream evolution of Λ-structure and turbulent spot on the smooth and ribbed surfaces are demonstrated, such as suppression by riblets of the Λ-vortex transformation into the turbulent spot, appearance of the coherent structures of Λ-vortex within ensemble-averaged turbulent spot, and oblique waves generation both by the Λ-vortex and turbulent spot. 相似文献19.
Particle image velocimetry technique has been used to investigate the evolution of synthesised vortical structures in the turbulent boundary layer. Synthetic jet actuator is implemented on the flat plate surface to synthesise various vortical structures by operating the actuator at varying operating parameters. The vortices are issued into the boundary layer and their evolution and subsequent interaction with the relatively less energetic near wall fluid is studied. The investigation is based on the quantitative measurements that are made both on the central and parallel lateral planes. Finally, the enhancement of the wall shear stress resulted in by the passing vortices is measured to evaluate the effectiveness of the actuator towards flow separation control. 相似文献
20.
高超声速后台阶流动是大气层内高速飞行器发动机设计、表面热防护以及高超声速拦截器红外成像窗口气动光学效应校正等诸多先进高超声速技术研发过程中所涉及的一类基础流动问题. 研究高超声速后台阶流动特性对有效提升飞行器综合性能, 进一步掌握高超声速流动机理具有重大基础 意义. 本文以二维高超声速后台阶流动为研究对象, 在KD-01高超声速激波风洞中测量了二维后台阶模型表面传热系数和表面静压, 并将实测台阶下游表面传热系数分布同采用高超声速边界层理论所得估计值进行了比较. 为进一步验证实验结果, 使用NPLS技术测量了其中一种实验状态下台阶周围流动结构. 研究发现, 对于二维高超声速后台阶流动, 台阶下游表面传热分布受台阶处边界层外缘流动特性的直接影响; 在台阶下游分离区和再附区内, 气体黏性占主导作用; 在台阶下游远场区域, 边界层流动特性趋同于平板边界层; 下游边界层基本结构取决于台阶处边界层相对厚度. 对高超声速后台阶流动, 若使用数值模拟方法研究气动热问题, 应当使用湍流模型. 相似文献