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Showing papers on "Starting vortex published in 2017"


Journal ArticleDOI
01 Jan 2017-Energy
TL;DR: In this article, the aerodynamic performance of the airfoil S809 without and with vortex generators was investigated using a computational fluid dynamic method of simulation, and the results were obtained with three-dimensional incompressible Reynolds-averaged Navier-Stokes equations.

91 citations


Journal ArticleDOI
TL;DR: In this article, the authors investigated the broadband noise generated by the scattering of turbulent flow at the trailing edge of a NACA 0018 airfoil with trailing edge serrations, varying both the angle of attack and serration flap angle.

62 citations


Journal ArticleDOI
TL;DR: In this paper, the authors presented a numerical study on a traditional Lapple cyclone separator with the inserted cross-shaped metal blades in the vortex finder, and the results showed that the inserted blades could decrease the pressure drop significantly while improving the separation efficiency slightly by 0.64%.

60 citations


Journal ArticleDOI
TL;DR: In this article, a NACA 0012 airfoil at Reynolds number 50 000 and angle of attack 5° with three different trailing edge shapes (straight, blunt, and serrated) was analyzed using dynamic mode decomposition.
Abstract: Direct numerical simulations of the flow field around a NACA 0012 airfoil at Reynolds number 50 000 and angle of attack 5° with 3 different trailing edge shapes (straight, blunt, and serrated) have been performed. Both time-averaged flow characteristics and the most dominant flow structures and their frequencies are investigated using the dynamic mode decomposition method. It is shown that for the straight trailing edge airfoil, this method can capture the fundamental as well as the subharmonic of the Kelvin-Helmholtz instability that develops naturally in the separating shear layer. The fundamental frequency matches well with relevant data in the literature. The blunt trailing edge results in periodic vortex shedding, with frequency close to the subharmonic of the natural shear layer frequency. The shedding, resulting from a global instability, has an upstream effect and forces the separating shear layer. Due to forcing, the shear layer frequency locks onto the shedding frequency while the natural freque...

55 citations


Journal ArticleDOI
TL;DR: In this paper, the relationship between the evolution of propeller trailing vortex wake and skew angle is numerically examined based on four different five-blade David Taylor Model Basin (DTMB) model propellers with different skew angles.

53 citations


Journal ArticleDOI
TL;DR: In this paper, a steady state numerical simulation is performed for investigating the thermal and fluid flow characteristics in a turbulent boundary layer for a flat channel as an element of a compact heat exchanger.

53 citations


Journal ArticleDOI
TL;DR: In this article, a biomimetic airfoil featuring leading edge waves, trailing edge serrations and surface ridges is proposed, based on flow control with each section meeting the NACA 0012 air-foil profile.

48 citations


Journal ArticleDOI
TL;DR: In this paper, an improved delayed detached eddy simulation (IDDES) method was adopted to investigate the effects of leading edge protuberances on airfoil stall and post-stall performance.
Abstract: This article presents a numerical investigation of the effects of leading-edge protuberances on airfoil stall and post-stall performance. An improved delayed detached eddy simulation (IDDES) method was adopted. As a result, to clarify the effects of ‘bi-periodic’ phenomenon around stall region, it was found that the flow separation at troughs was the main inducement of aerodynamic lift degradation within pre-stall regime and the flow pattern where vortices diverged was predominant. It was also found that the variations in flow patterns led to the gentle stall process. Furthermore, to study the statistical characteristics of unsteady vortex shedding, corresponding spectrum characteristics were also analyzed from another perspective, suggesting that the vortex shedding frequency was higher where vortices converged. Eventually, the improved performances of tubercled airfoil within post-stall regime could be attributed to the strong streamwise vortices generated by the leading-edge protuberances. Depl...

45 citations


Journal ArticleDOI
TL;DR: In this paper, the authors introduced a novel visualization technique with instrumented guide vanes embedding the visualization devices, providing unprecedented views on the inter-blade cavitation vortex, which is a typical cavitation phenomenon observed at deep part load operation.
Abstract: Francis turbines are subject to various types of cavitation flow depending on the operating condition. To enable a smooth integration of the renewable energy sources, hydraulic machines are now increasingly required to extend their operating range, especially down to extremely low discharge conditions called deep part load operation. The inter-blade cavitation vortex is a typical cavitation phenomenon observed at deep part load operation. However, its dynamic characteristics are insufficiently understood today. In an objective of revealing its characteristics, the present study introduces a novel visualization technique with instrumented guide vanes embedding the visualization devices, providing unprecedented views on the inter-blade cavitation vortex. The binary image processing technique enables the successful evaluation of the inter-blade cavitation vortex in the images. As a result, it is shown that the probability of the inter-blade cavitation development is significantly high close to the runner hub. Furthermore, the mean vortex line is calculated and the vortex region is estimated in the three-dimensional domain for the comparison with numerical simulation results. In addition, the on-board pressure measurements on a runner blade is conducted, and the influence of the inter-blade vortex on the pressure field is investigated. The analysis suggests that the presence of the inter-blade vortex can magnify the amplitude of pressure fluctuations especially on the blade suction side. Furthermore, the wall pressure difference between pressure and suction sides of the blade features partially low or negative values near the hub at the discharge region where the inter-blade vortex develops. This negative pressure difference on the blade wall suggests the development of a backflow region caused by the flow separation near the hub, which is closely related to the development of the inter-blade vortex. The development of the backflow region is confirmed by the numerical simulation, and the physical mechanisms of the inter-blade vortex development is, furthermore, discussed.

41 citations


Journal ArticleDOI
TL;DR: In this article, the authors studied the compressible starting jet numerically and found that the interaction strongly links the vortex ring and the trailing jet in the incompressible case and showed that compressibility reduces the critical Reynolds number for the interaction.
Abstract: The dominant feature of the compressible starting jet is the interaction between the emerging vortex ring and the trailing jet. There are two types of interaction: the shock–shear layer–vortex interaction and the shear layer–vortex interaction. The former is clearly not present in the incompressible case, since there are no shocks. The shear layer–vortex interaction has been reported in the literature in the incompressible case and it was found that compressibility reduces the critical Reynolds number for the interaction. Four governing parameters describe the compressible starting jet: the non-dimensional mass supply, the Reynolds number, the reservoir to unbounded chamber temperature ratio and the reservoir to unbounded chamber pressure ratio. The latter parameter does not exist in the incompressible case. For large Reynolds numbers, the vortex pinch-off takes place in a multiple way. We studied the compressible starting jet numerically and found that the interaction strongly links the vortex ring and the trailing jet. The shear layer–vortex interaction leads to a rapid breakdown of the head vortex ring when the flow impacted by the Kelvin–Helmholtz instabilities is ingested into the head vortex ring. The shock–shear layer–vortex interaction is similar to the noise generation mechanism of broadband shock noise in a continuously blowing jet and results in similar sound pressure amplitudes in the far field.

41 citations


Journal ArticleDOI
TL;DR: In this article, high-speed flow visualization is complemented by quantitative velocity and surface pressure measurements to study vortex shedding within laminar separation bubbles forming over the suction side of a NACA 0018 airfoil.
Abstract: Vortex shedding within laminar separation bubbles forming over the suction side of a NACA 0018 airfoil is studied through a combination of high-speed flow visualization and boundary layer measurements. Wind tunnel experiments are performed at a chord-based Reynolds number of 100,000 and four angles of attack. The high-speed flow visualization is complemented by quantitative velocity and surface pressure measurements. The structures are shown to originate from the natural amplification of small-amplitude disturbances, and the shear layer roll-up is found to occur coherently across the span. However, significant cycle-to-cycle variations are observed in vortex characteristics, including shedding period and roll-up location. The formation of the roll-up vortices precedes the later stages of transition, during which these structures undergo significant deformations and breakdown to smaller scales. During this stage of flow development, vortex merging is also observed. The results provide new insight into the development of coherent structures in separation bubbles and their relation to the overall bubble dynamics and mean bubble topology.

Journal ArticleDOI
TL;DR: In this paper, the formation and evolution characteristics of the continuously generated vortical structure and resulting flow field in quiescent air induced by a dielectric-barrier discharge (DBD) plasma actuator in burst mode operation are reported.
Abstract: The present study reports the formation and evolution characteristics of the continuously generated vortical structure and resulting flow field in quiescent air induced by a dielectric-barrier-discharge (DBD) plasma actuator in burst mode operation. A starting vortex is formed during the initial actuation period, which disappears after a small time interval for continuous mode operation of the DBD plasma actuator. A burst input signal to the actuator generates a train of self-similar vortices. The behaviour of vortices and the average flow field induced by the actuator has been studied using high speed schlieren visualization and particle image velocimetry technique for different actuation amplitude and duty cycle parameters. These repeating vortices travel faster than the starting vortex, and the vortex core velocity of these repeating vortices increases with increase in duty cycle parameter. Fuller u-velocity profile, higher v-velocity near the edge of the outer shear layer region, and higher growth of ...

Journal ArticleDOI
TL;DR: In this article, the influence of exit orifice shape on the performance characteristics of a three-electrode plasma synthetic jet actuator was investigated in quiescent conditions using high-speed Schlieren imaging and phase-locked two-component PIV measurements.
Abstract: This study experimentally investigates the influence of exit orifice shape on the performance characteristics of a three-electrode plasma synthetic jet actuator. High-speed Schlieren imaging system and phase-locked two-component PIV measurements are used for flowfield characterisation in quiescent conditions. Two actuator configurations with the same exit area but different exit orifice shape (round orifice and slot orifice) are studied. Results indicate a close correspondence between the shapes of the starting vortex ring with the shapes of the respective exit orifices. For the slot orifice, the elongated starting vortex ring gradually expands during propagation, while its ends become warped. A distinct K–H instability structure is observed, inducing continuous oscillation of the high-speed jet. Compared with the jet from the round orifice, the slot jet has a higher entrainment rate of surrounding air, thus resulting in a lower propagation velocity of the jet front. The exit velocity of PSJA within one period initially shows a rapid increase, then persists at a relatively high level (100–130 m/s), and finally drops with some small-scale oscillations. The oscillation amplitude is less than 10 m/s, and the oscillation period is approximately 600 µs. Under conditions of same exit area, orifice shape has little influence on the variation of the exit velocity.

Journal ArticleDOI
TL;DR: In this article, the formation of afterbody vortex flows from cylindrical bodies with a slanted base, whose upsweep angle was varied between 24° and 32°, was studied.
Abstract: Experiments have been undertaken to study the formation of afterbody vortex flows from cylindrical bodies with a slanted base, whose upsweep angle was varied between 24° and 32°. Vortex roll-up is mostly completed in the first half of the upswept section, where the vortex causes largest suction on the surface. Towards the trailing-edge the vortices become more axisymmetric and stronger with increasing upsweep angle. Although there is some delay in vortex roll-up at lower Reynolds number, the main features of the vortex flow are similar to those at higher Reynolds number. The strength of the vortices at the trailing-edge was proportional to the time-averaged drag coefficient, which increased by nearly 50% in the range of upsweep angles tested. The vortex was more coherent with reduced meandering and a smaller core radius towards the trailing-edge. This reduction in meandering along the streamwise direction had not been observed previously with other external vortex flows in aerodynamics. Proper Orthogonal Decomposition revealed that the helical displacement mode with azimuthal wavenumber m = 1 was the dominant mode towards the trailing-edge, suggesting that the afterbody vortices bear much similarity with the more widely studied wing tip vortices and delta wing vortices. The instantaneous vortex pair exhibits time-dependent asymmetry; however, there is virtually no correlation between the displacements of the vortex centers.

Journal ArticleDOI
TL;DR: In this article, the turbulent flow around a circular cylinder has been investigated at R e = 5000 using direct numerical simulations, and two instability mechanisms were found to coexist in the present case study: a global type instability originating in the shear layer, which shows a characteristic frequency, and a convective type instability that seems to be constantly present in the near wake.

Journal ArticleDOI
TL;DR: In this article, a frequency response approach is taken to model unsteady aerodynamics resulting from plunging oscillations of an airfoil, with particular attention paid to the flow separation and consequent formation and convection of the leading edge vortex.

Journal ArticleDOI
TL;DR: In this article, a two-phase fluid mechanical modeling method for ladle teeming was proposed, where a dynamic model for vortex suction process was built, and the profiles of vortex flow field were acquired.
Abstract: At the late stage of continuous casting (CC) ladle teeming, sink vortex can suck the liquid slag into tundish, and cause negative influences on the cleanliness of molten steel. To address this issue, a two-phase fluid mechanical modeling method for ladle teeming was proposed. Firstly, a dynamic model for vortex suction process was built, and the profiles of vortex flow field were acquired. Then, based on the level set method (LSM), a two-phase 3D interface coupling model for slag entrapment was built. Finally, in combination with high-order essentially non-oscillatory (ENO) and total variation diminishing (TVD) methods, a LSM-based numerical solution method was proposed to obtain the 3D coupling evolution regularities in vortex suction process. Numerical results show that the vortex with higher kinetic energy can form an expanded sandglass-shape region with larger slag fraction and lower rotating velocity; there is a pressure oscillation phenomenon at the vortex penetration state, which is caused by the energy shock of two-phase vortex penetration coupling.

Journal ArticleDOI
TL;DR: In this paper, the size of the primary vortex generated by a single VG on a flat plate by Computational Fluid Dynamics simulations using OpenFOAM code is characterized by assessing the half-life radius of the vortex and comparing it with experimental results.

Journal ArticleDOI
TL;DR: In this article, a canonical geometry was developed to investigate the flow and heat transfer of a purely oscillatory jet that is not influenced by the manner by which it is produced, and a definition of the jet characteristic velocity was developed rigorously based on the vortex dynamics produced by the jet.

Journal ArticleDOI
27 Oct 2017-Energies
TL;DR: In this paper, the influence of tip vortex on wind turbine wake by Computational Fluid Dynamics (CFD) simulations is investigated, and the wind velocities obtained by CFD simulations are also compared with the experimental data from wind tunnel experiments.
Abstract: Wind velocity distribution and the vortex around the wind turbine present a significant challenge in the development of straight-bladed vertical axis wind turbines (VAWTs). This paper is intended to investigate influence of tip vortex on wind turbine wake by Computational Fluid Dynamics (CFD) simulations. In this study, the number of blades is two and the airfoil is a NACA0021 with chord length of c = 0.265 m. To capture the tip vortex characteristics, the velocity fields are investigated by the Q-criterion iso-surface (Q = 100) with shear-stress transport (SST) k-ω turbulence model at different tip speed ratios (TSRs). Then, mean velocity, velocity deficit and torque coefficient acting on the blade in the different spanwise positions are compared. The wind velocities obtained by CFD simulations are also compared with the experimental data from wind tunnel experiments. As a result, we can state that the wind velocity curves calculated by CFD simulations are consistent with Laser Doppler Velocity (LDV) measurements. The distribution of the vortex structure along the spanwise direction is more complex at a lower TSR and the tip vortex has a longer dissipation distance at a high TSR. In addition, the mean wind velocity shows a large value near the blade tip and a small value near the blade due to the vortex effect.

Journal ArticleDOI
TL;DR: In this article, it was shown that with dynamic airfoil deformation the propulsion efficiency can be improved considerably and with increasing plunge amplitude the flow on the flapping wing starts to separate and concentrated dynamic stall vortex may develop on both upper and lower wing surfaces.

Journal ArticleDOI
TL;DR: In this article, a 2D unsteady numerical simulation with dynamic and sliding meshing techniques was conducted to solve the flow around a three-blade Vertical axis wind turbine (VAWT).
Abstract: A 2D unsteady numerical simulation with dynamic and sliding meshing techniques was conducted to solve the flow around a threeblade Vertical axis wind turbine (VAWT). The circular wakes, strip-like wakes and the shedding vortex structures interact with each other result in an extremely unstable performance. An airfoil with a trailing edge flap, based on the NACA0012 airfoil, has been designed for VAWT to improve flow field around the turbine. Strategy of flap control is applied to regulate the flap angle. The results show that the flapped airfoil has an positive effect on damping trailing edge wake separation, deferring dynamic stall and reducing the oscillating amplitude. The circular wake vortices change into strip vortices during the pitch-up interval of the airfoils. Examination of the flow details around the rotating airfoil indicates that flap control improves the dynamic stall by diminishing the trend of flow separation. Airfoil stall separation has been suppressed since the range of nominal angle of attack is narrowed down by an oscillating flap. Vortices with large intensity over rotational region are reduced by 90 %. The lift coefficient hysteresis loop of flapped airfoil acts as an O type, which represents a more stable unsteady performance. With flap control, the peak of power coefficient has increased by 10 % relative to the full blade VAWT. Obviously, the proposed flapped airfoil design combined with the active flow control significantly has shown the potential to eliminate dynamic stall and improve the aerodynamic performance and operation stability of VAWT.

Journal ArticleDOI
TL;DR: In this paper, a mathematical model that invokes the Kutta condition to account for vortex shedding from the trailing edge of a free hydrofoil in a planar ideal fluid is compared with a canonical model for the dynamics of a terrestrial vehicle subject to a nonintegrable velocity constraint.
Abstract: A mathematical model that invokes the Kutta condition to account for vortex shedding from the trailing edge of a free hydrofoil in a planar ideal fluid is compared with a canonical model for the dynamics of a terrestrial vehicle subject to a nonintegrable velocity constraint. The Kutta condition is shown to be nonintegrable in a sense that parallels that in which the constraint on the terrestrial vehicle is nonintegrable. Simulations of the two system’s dynamics reinforce the analogy between the two.

Journal ArticleDOI
TL;DR: In this paper, the thermal-fluid characteristics of a pin-fin heat sink with delta winglet vortex generators in a cross flow were investigated experimentally and numerically, and it was determined that an angle of attack of 30° is a better arrangement for the vortex generators.

Journal ArticleDOI
04 Aug 2017-Science
TL;DR: On page 487 of this issue, Scheeler et al. (3) explore a particular property of a vortex ring whose core is helical rather than circular in form, an integral over the fluid domain that expresses the correlation between velocity and vorticity.
Abstract: The vortex ring is a fundamental phenomenon of fluid dynamics, recognized since the seminal investigations of Helmholtz ( 1 ) and Kelvin ( 2 ). Its familiar manifestation as a “smoke ring” in air derives from the fact that both smoke and vorticity (local fluid spin) are transported with the flow, which is “induced” by the vortex itself; so the smoke provides a natural visualization of the vorticity (see the photo). Vortex rings can also be generated in water and visualized either by dye or by small air bubbles that migrate to the low-pressure region at the core of the vortex. On page 487 of this issue, Scheeler et al. ( 3 ) explore a particular property of a vortex ring whose core is helical rather than circular in form. This property, helicity, is an integral over the fluid domain that expresses the correlation between velocity and vorticity, and an invariant of the classical Euler equations of ideal (inviscid) fluid flow. The question addressed by Scheeler et al. is the extent to which the helicity remains invariant when fluid viscosity, unavoidable in reality, is taken into consideration.

Journal ArticleDOI
TL;DR: In this paper, a series of metal rods and metal blades are inserted in the typical Lapple cyclone separator to reduce the intensity of the inner vortex, and the results show that when the length of the metal blades is less than the boundary between the inner and outer vortexes, that is, the outer vortex remains unchanged and inner vortex is destroyed partly, the separation efficiency remains constant and the pressure drop significantly decreases.
Abstract: The inner vortex plays a key role in the performance of cyclone separators. To explore the function and effect of the inner vortex in cyclone separators, a series of metal rods and metal blades are inserted in the typical Lapple cyclone separator to reduce the intensity of the inner vortex. First, the changes in general performance of cyclones are measured by experimental methods after insertion of the metal rods and metal blades. The flow field and particle motion are then simulated, respectively, by means of a Reynolds stress model (RSM) and a Lagrangian particle tracking (LPT) model. The results show that when the length of the metal blades is less than the boundary between the inner and outer vortexes, that is, the outer vortex remains unchanged and the inner vortex is destroyed partly, the separation efficiency remains constant and the pressure drop significantly decreases. When the length of the metal blades exceeds the boundary, the inner vortex is completely destroyed, and the outer vortex is significantly damaged, which results in sharp decrease of both the separation efficiency and pressure drop. The results indicate that the inner vortex has a notable effect on the pressure drop and virtually none on the separation efficiency. © 2017 American Institute of Chemical Engineers AIChE J, 63: 4508–4518, 2017

Journal ArticleDOI
TL;DR: In this paper, the authors investigated the influence of the shape of the ground obstacles on dissipating wake vortex in the present work, and showed that the resulting drag force acting on the obstacle has a more direct effect on wake dissipation.

Journal ArticleDOI
TL;DR: In this article, a simple momentum injection based active flow control strategy was proposed to suppress vortex induced oscillations at low Reynolds numbers, where two small control cylinders behind the main cylinder played the role of actuators, enforcing the desired momentum injection.

Journal ArticleDOI
TL;DR: In this article, an investigation of symmetry breaking and naturally occurring instabilities over thin slender delta wings with sharp leading edges was carried out in a water tunnel using particle image velocimetry (PIV) measurements.
Abstract: An investigation of symmetry breaking and naturally occurring instabilities over thin slender delta wings with sharp leading edges was carried out in a water tunnel using particle image velocimetry (PIV) measurements. Time-averaged location, strength and core radius of conical vortices vary almost linearly with chordwise distance for three delta wings with , and sweep angles over a wide range of angles of attack. Properties of the time-averaged vortex pairs depend only on the similarity parameter, which is a function of the angle of attack and the sweep angle. It is shown that time-averaged vortex pairs develop asymmetry gradually with increasing values of the similarity parameter. Vortex asymmetry can develop in the absence of vortex breakdown on the wing. Instantaneous PIV snapshots were analysed using proper orthogonal decomposition and dynamic mode decomposition, revealing the shear layer and vortex instabilities. The shear layer mode is the most periodic and more dominant for lower values of the similarity parameter. The Strouhal number based on the free stream velocity component in the cross-flow plane is a function of only the similarity parameter. The dominant frequency of the shear layer mode decreases with the increasing similarity parameter. The vortex modes reveal the fluctuations of the vorticity magnitude and helical displacement of the cores, but with little periodicity. There is little correlation between the fluctuations in the cores of the vortices.

Journal ArticleDOI
TL;DR: In this article, a 3D wake transition for a circular cylinder placed near to a moving wall is investigated using direct numerical simulation (DNS), covering a parameter space spanning a gap ratio and Reynolds number up to 325.
Abstract: Three-dimensional (3D) wake transition for a circular cylinder placed near to a moving wall is investigated using direct numerical simulation (DNS). The study covers a parameter space spanning a gap ratio and Reynolds number ( ) up to 325. The wake transition regimes in the parameter space are mapped out. It is found that vortex dislocation associated with Mode A is completely suppressed at smaller than approximately 1.0. The suppression of vortex dislocation is believed to be due to the confinement of the Mode A streamwise vortices by the plane wall, which suppresses the excess growth and local dislocation of any Mode A vortex loop. Detailed wake transition is examined at , where the wake transition sequence is ‘two-dimensional (2D) ordered Mode A mode swapping (without dislocations) Mode B’. Relatively strong three-dimensionality is found at as the wake is dominated by large-scale structure of ordered Mode A, and also at , where Mode B becomes increasingly disordered. A local reduction in three-dimensionality is observed at , where the wake is dominated by finer-scale structure of a mixture of ordered Modes A and B. Corresponding variations in the vortex shedding frequency and hydrodynamic forces are also investigated.