23 research outputs found

    Experimental and numerical investigation of blade–tower interaction noise

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    © 2018 Elsevier Ltd. This manuscript version is made available under the CC-BY-NC-ND 4.0 license: http://creativecommons.org/licenses/by-nc-nd/4.0/ This author accepted manuscript is made available following 12 month embargo from date of publication (December 2018) in accordance with the publisher’s archiving policyThis paper describes the generation of blade–tower interaction (BTI) noise from upwind turbines and pylon-mounted fans using a combination of experimental and numerical means. An experimental rotor-rig was used in an anechoic chamber to obtain BTI acoustic data under controlled conditions. A computational model, based on the solution of the unsteady Reynolds Averaged Navier Stokes (URANS) equations and Curle's acoustic analogy, was used to describe the generation of fan and simplistic model of wind turbine BTI noise by the rotor-rig. For both the fan and model wind turbine case, the tower was found to be a more significant source of BTI noise than rotor blades. The acoustic waveforms for both turbine and fan are similar; however, in the case of the turbine, the blade contribution reinforces that from the tower, while in the case of a fan, there is some cancellation between the tower source and the blade source. This behavior can be explained by the unsteady aerodynamics occurring during BTI

    Flat-Plate Interaction with the Near Wake of a Square Cylinder

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    An infinitely thin flat plate placed in the near wake of a square cylinder at a Reynolds number of Re = 150 was studied. The two-dimensional incompressible Navier-Stokes equations were solved using the finite volume OpenFOAM numerical simulation system. The pressure-implicit split-operator algorithm with two correction steps was used as an implicit transient-solution scheme. The resulting system of equations was solved using the incomplete Choleski conjugate gradient method with a solution tolerance of 10 -6. All simulations were performed at Re = 150, making a two-dimensional study appropriate. Two computational domains were constructed for this study, and an inlet boundary condition was applied to the upstream boundary in each of them. The result showed that the force on the square cylinder was reduced significantly and the amplitude of the lift coefficient on the downstream plate was found to be the same as for the single square cylinder.Con J. Doola

    Flow around a square cylinder with a detached downstream flat plate at a low Reynolds number

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    This paper investigates the interaction of a square cylinder wake with a detached flat plate of length equal to one cylinder height (D) at various downstream locations (G). Two modes of wake-plate interaction are observed from this study. For short gaps (G ≲ 2D), a shear layer-plate interaction is observed, where the first flow regime is generated. In this regime, the shear layers roll up downstream of the plate. The optimal location of the plate is found at G ≲ 2D for maximum reductions in fundamental vortex shedding frequency, root mean square lift and mean drag of the cylinder. A sudden jump in Strouhal number is observed between 2D ≲ G ≲ 2:5D, which suggests a transition into a new mode of wake-plate interaction. For long gaps (2:5D ≲ G ≲ 5D), a vortex-plate interaction is observed, where the second flow regime is generated. In this regime, the shear layers roll up within the gap, and the flow structure at near to the cylinder is almost unchanged with the gap

    Aeolian tones generated by a square cylinder with a detached flat plate

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    A possibility of a rigid flat plate that is placed in the wake of a square cylinder for a passive sound control is investigated numerically. The changes in the sound generation with gap distances are inspected at a Reynolds number of 150 and a Mach number of 0.2 for a constant plate length of D. Two regimes that significantly effects the sound generation are identified. The first regime, i.e. pre-vortex regime, is for 0 G 2.3D and the second regime, i.e. post-vortex regime, is for 2.4D G 7D. A sound reduction can be obtained in pre-vortex regime, where about 2.9 dB sound reduction is obtained when there is no gap between the two bodies. Contrary, at least an increase 8.0 dB sound level is emitted when the plate is placed in the post-vortex regime. Despite of that, a 6.3 dB sound reduction is obtained when the plate length is reduced to 0.26D and placed at 5.6D downstream of the cylinder. The sound reduction is limited by the deformation in the sinusoidal signal of the plate due to the unsteady plate stall process

    The effect of acoustic forcing on an airfoil tonal noise mechanism

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    Hybrid Artificial Boundary Conditions for the Application of Blunt-Body Aerodynamic Noise Prediction

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    A hybrid artificial boundary condition (HABC) that combines the volume-based acoustic damping layer (ADL) and the local face-based characteristic boundary condition (CBC) is presented to enhance the absorption of acoustic waves near the computational boundaries. This method is applied to the prediction of aerodynamic noise from a circular cylinder immersed in uniform compressible viscous flow. Different ADLs are designed to assess their effectiveness whereby the effect of the mesh-stretch direction on wave absorption in the ADL is analysed. Large eddy simulation (LES) and FW-H acoustic analogy method are implemented to predict the far-field noise, and the sensitivities of each approach to the HABC are compared. In the LES computed propagation field of the fluctuation pressure and the frequency-domain results, the spurious reflections at edges are found to be significantly eliminated by the HABC through the effective dissipation of incident waves along the wave-front direction in the ADL. Thereby, the LES results are found to be in a good agreement with the acoustic pressure predicted using FW-H method, which is observed to be just affected slightly by reflected waves

    Transient interaction between a reaction control jet and a hypersonic crossflow

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    This paper presents a numerical study that focuses on the transient interaction between a reaction control jet and a hypersonic crossflow with a laminar boundary layer. The aim is to better understand the underlying physical mechanisms affecting the resulting surface pressure and control force. Implicit large-eddy simulations were performed with a round, sonic, perfect air jet issuing normal to a Mach 5 crossflow over a flat plate with a laminar boundary layer, at a jet-to-crossflow momentum ratio of 5.3 and a pressure ratio of 251. The pressure distribution induced on the flat plate is unsteady and is influenced by vortex structures that form around the jet. A horseshoe vortex structure forms upstream and consists of six vortices: two quasi-steady vortices and two co-rotating vortex pairs that periodically coalesce. Shear-layer vortices shed periodically and cause localised high pressure regions that convect downstream with constant velocity. A longitudinal counter-rotating vortex pair is present downstream of the jet and is formed from a series of trailing vortices which rotate about a common axis. Shear-layer vortex shedding causes periodic deformation of barrel and bow shocks. This changes the location of boundary layer separation which also affects the normal force on the plate.</p

    Numerical investigation of a pulsed reaction control jet in hypersonic crossflow

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    This paper presents a numerical study on the flow structures developed when a pulsed reaction control jet is operated in a hypersonic crossflow with a laminar boundary layer. Understanding these flow structures is important to the design of reaction control jets and scramjet fuel injectors. Implicit large-eddy simulations were performed with a round, sonic, perfect air jet issuing normal to a Mach 5 crossflow over a flat plate, at a jet-to-crossflow momentum ratio of 5.3 and a pressure ratio of 251, and with square-wave pulsing at Strouhal numbers of 1/6 to 1/3, based on jet diameter and free-stream velocity. Pulsing the jet allows the shock structure to partially collapse when the jet is off. This shock collapse affects the shedding frequency of shear-layer vortices, the formation of shear-layers downstream of the jet outlet, and the formation of longitudinal counter-rotating vortices. The lead shocks formed at jet start-up allow deeper penetration by increasing the effective jet-to-crossflow momentum ratio near the jet outlet and by preventing interaction between hairpin vortices. Normalised penetration was increased by a maximum of 68% compared with the steady jet. Pulsing also provides a higher jet interaction force per unit mass flow rate compared with a steady jet, with a 52% increase recorded at a 33% duty cycle. Temporal and spatial variations of surface pressure are important for reaction control applications and have been quantified. Pressure distribution depends strongly on duty cycle, and higher interaction force per unit mass flow rate was observed in cases with low duty cycle.</p
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