Analytical and Numerical Methods in Vortex-Body Aeroacoustics

Total Page:16

File Type:pdf, Size:1020Kb

Analytical and Numerical Methods in Vortex-Body Aeroacoustics Numéro d'ordre :2002-13 ANNÉE 2002 THÈSE présentée devant le POLITECNICO DI TORINO etl'ÉCOLE CENTRALE DE LYON pour obtenir le double titreItalo-Français et le titre Européen de DOCTEUR spécialité MÉCANIQUE DES FLUIDES et ACOUSTIQUE par Damiano CASALINO ANALYTICAL AND NUMERICAL METHODS IN VORTEX-BODY AEROACOUSTICS Soutenue le 8 avril 2002 devatit la Commissiond'Examen JURY Président: Prof.A. COGHE Examinateurs : Prof.M. ROGER Dr. M. JACOB Prof.G. P. ROMANO Prof.E. CARRERA Rapporteurs: Prof.M. HIRSCHBERG Prof.W. SCHRODER Dipartimento di Ingegneria Aeronautica e Spaziale Politecnico di Torino et Laboratoire de Mécanique des Fluides et d'Acoustique, UMR CNRS 5509 Ecole Centrale de Lyon Numéro d'ordre : 2002-13 ANNÉE 2002 THÈSE présentée devant le POLITECNICO DI TORINO et l'ÉCOLE CENTRALE DE LYON pour obtenir le double titre Italo-Français et le titre Européen de DOCTEUR spécialité MÉCANIQUE DES FLUIDES et ACOUSTIQUE par Damiano CASALINO ANALYTICAL AND NUMERICAL METHODS IN VORTEX-BODY AEROACOUSTICS Soutenue le 8 april 2002 devant la Commission d'Examen JURY Président: Prof.A. COGHE Examinateurs: Prof.M. ROGER Dr. M. JACOB Prof.G. P. ROMANO Prof.E. CARRERA Rapporteurs: Prof.M. HIRSCHBERG Prof.W. SCHRÖDER Dipartimento di Ingegneria Aeronautica e Spaziale Politecnico di Torino et Laboratoire de Mécanique des Fluides et d'Acoustique, UMR CNRS 5509 Ecole Centrale de Lyon -r Ecole Centralede Lyon BtBLIOTHEQUE 36, avenue GuydeCoUOflgUe F - 69134ECULLY CEDEX Preface This work deals with that branch of Aeroacoustics concerning the noise generated by the interaction between vortical flows and rigid surfaces.It is the outcome of a PhD research shared among the Dipartimento di Ingegneria Aeronautica e Spaziale at Politecnico di Torino and the Laboratoire de Mécanique des Fluides et d'Acoustique at Ecole Centrale de Lyon. Results concerning a nominal two-dimensional flow, the rod-airfoil configuration,are brought to- gether with a description of the noise generation mechanisms in fluid-body interactions. The rod-airfoil configuration is the object of part I, where I summarizedmy analytical contribu- tions to the vortex-airfoil interaction problem and to the development of numerical methodologies of aeroacoustic prediction. The description of the sound generation mechanisms in fluid-body interactions is the object of part II. This constitutes the theoretical basis on which I founded my PhD education. Therefore, part I constitutes my PhD Thesis and part II should be assumed as formally separated by part I. However, because of the great engagement required by writing part H, my opinion and feeling are to include it in the present work and to consider part I and part II as substantially joined. Of course, part I is in its definitive form, because it represents the outcome of a time constrained research. On the contrary, thanks to its formal autonomy, part II will be reviewed in the next future. Damiano Casalino i Contents IInteraction Noise from an Airfoil in the Wake ofa Cylinder 9 iIntroduction 13 1.1A Brief Description of the Vortex Dynamics in a Rod-Airfoil Configuration 14 1.2Theoretical and Practical Relevance of the Rod-Airfoil Configuration 15 1.3Part I Overview 16 2 Vortex-Airfoil Interaction: Aerodynamic Modeling 19 2.1Introduction 20 2.2The Aerodynamic Problem 22 2.2.1Flow Model 23 2.2.2The Kutta Condition and the Physical Role of Vortex Shedding 26 2.2.3A Fixed-Wake Formulation of the Vortex-Airfoil Interaction Problem 27 2.2.4The Oncoming Vortex Trajectory 30 2.2.5 A Free-Wake Formulation of the Vortex-Airfoil Interaction Problem 30 2.2.6The Cloud of Oncoming Vortices 33 2.2.7The Double Row of Counter-Rotating Vortices 36 2.2.8The Aerodynamic Force on the Airfoil 38 2.3Conclusions 39 3Vortex-Airfoil Interaction: Acoustic Modeling 53 3.1Acoustic Analogy Approach 53 3.2Aeroacoustic Sources 54 3.3A Linear Model for the Vortex-Airfoil Interaction Noise 55 3.4A Matched Asymptotic Expansion Model of the Vortex-Airfoil Interaction Noise 59 3.4.1 Inner Problem 60 3.4.2 Outer Problem 61 3.4.3Solution and Matching 62 3.4.4Discussion 66 3.5Conclusions 67 4 Vortex-Airfoil Interaction: Results and Discussion 69 4.1Effects of the Vortex Convection Velocity 69 4.1.1 Aerodynamic Results 70 4.1.2 Acoustic Results 72 4.1.3 Comparisons with Howe's Analytical Model 72 4.2Effects of the Vortex Distortion 75 4.2.1 Aerodynamic Results 75 4.2.2Acoustic Results 76 4.2.3An Example of Vortex Splitting 78 4.3Effects of the Airfoil Camber 80 3 4 CONTENTS 4.3.1 Aerodynamic Results 80 4.3.2 Acoustic Results 81 4.4The Unsteady Pressure Field on the Airfoil Surface 84 4.4.1Trailing Edge Behaviour 84 4.4.2 Aeroacoustic Sources Characterization 85 4.5Effects of the Free-Stream Velocity 90 4.5.1 Aerodynamic Results 90 4.5.2Acoustic Results 91 4.6Effects of the Airfoil Angle of Attack 93 4.6.1Aerodynamic Results 93 4.6.2Acoustic Results 93 4.7Comparison with Experimental Results 97 4.7.1Aerodynamic Results 97 4.7.2Acoustic Results 99 4.8Conclusions 102 5Rod-Airfoil Experiment 103 5.1Experimental Set-Up 103 5.1.1 Acoustic Measurements 103 5.1.2Surface Pressure Measurements 104 5.2Experimental Results 104 5.2.1 Acoustic Measurements 105 5.2.1.1 Isolated rod noise 105 5.2.1.2 Rod-airfoil configuration noise 107 5.2.1.3 Airfoil noise 107 5.2.2Spatial Coherence and Correlation Measurements 113 5.2.2.1 Rod configuration 113 5.2.2.2 Rod-airfoil configuration 118 5.3A Hydrogen Bubble Visualization Experiment 127 5.4Conclusions 131 6 Acoustic Analogy Formulation 139 6.1 Introduction 139 6.2Aeroacoustic Formulation 141 6.2.1 The FW-H Equation 141 6.2.2The FW-H Equation versus the Kirchhoff Equation 143 6.2.3The Retarded Time Formulation of the FW-H Equation 144 6.2.3.1 Non-dimensionalized FW-H Integral Equation 148 6.2.4The Advanced Time Fornmlation 149 6.3Numerical Assessment of Advanlia 152 6.3.1 Two-dimensional Tests 152 6.3.1.1 Test 1 152 6.3.1.2 Test 2 155 6.3.2Three-dimensional Tests 156 6.3.2.1 Test 1 156 6.3.2.2 Test 2 162 6.3.2.3 Test 3 166 6.3.3Discussion 169 6.4On the Feasibility of a Hybrid CFD/FW-H Aeroacoustic Prediction 169 6.5Conclusions 169 CONTENTS 5 7 Spanwise Statistical Modeling of a Circular Cylinder Flow 177 7.1Introduction 177 7.2Vortex Dynamics in the a Wake of a Circular Cylinder 178 7.2.1Three-Dimensional Effects 180 7.2.1.1 Three-Dimensionality at Low Reynolds Numbers 180 7.2.1.2 Three-Dimensionality at High Reynolds Numbers 181 7.3A Statistical Method for Aeroacoustic Predictions 182 7.3.1Phillips' Model 182 7.3.2The Method of the Phase Variance Distribution 183 7.3.3Random Amplitude Modulation versus Spanwise Phase Dispersion 187 7.3.4Aeroacoustic Implementation of the Statistical Model 188 7.4Aeroacoustic Prediction of a Circular Cylinder Flow 188 7.4.1 Aerodynamic Computation 188 7.4.2Acoustic Computation 189 7.4.3Aerodynamic Results 189 7.4.4Acoustic Results 192 7.5Conclusions 198 8 RANS/FW-H Rod-Airfoil Aeroacoustic Prediction 201 8.1Introduction 201 8.2On the Adequacy of a Hybrid RANS/FW-H Aeroacoustic Prediction 204 8.3The Rod-Airfoil Aerodynamic Simulation 205 8.3.1The Aerodynamic Solver 205 8.3.2Computational Parameters 205 8.3.3Flow Parameters and Initial Conditions 206 8.3.4Geometrical Parameters 206 8.3.5 Computational Mesh 207 8.4The Rod-Airfoil Acoustic Computation 207 8.5Results and Discussion 210 8.5.1 Aerodynamic Results 210 8.5.1.1 Unsteady force on the airfoil and wall pressure field 210 8.5.1.2 Airfoil results versus rod results 214 8.5.1.3 Mean and fluctuating flow near the airfoil 216 8.5.1.4 Mean and fluctuating flow past the cylinder 217 8.5.1.5 Snapshots of the Rod-Airfoil Aerodynamic Field 225 8.5.2 Acoustic Results 234 8.5.2.1 Influence of the integration surface 234 8.5.2.2 Comparison with acoustic measurements 235 8.5.2.3 Effects of the airfoil angle of attack 238 8.6Conclusions 243 9 Epilogue of part I 245 IIAerodynamic Noise in Fluid-Body Interactions 247 1Basic Equations of Fluid Mechanics 251 1.1 Introduction 251 1.2Reynolds' Transport Theorem 251 1.3Governing Equations of Fluid Motion 253 6 CONTENTS 1.3.1 The Continuity Equation 253 1.3.2The Momentum Equation 254 1.3.3The Energy Equation 258 1.3.4Convective Form of the Flow Governing Equations 259 1.4Potential Flows 260 1.4.1 Green's Functions of Wave Equations 264 1.5The Helmholtz Decomposition 265 2Nonlinearity and Modes of Fluctuation 267 2.1Introduction 267 2.2 A Perturbative Expansion of the Navier-Stokes Equations 267 2.3Physics of Modal Bilateral Interaction 274 3 The Pressure Field at the Wall of a Turbulent Boundary-Layer 277 3.1Introduction 277 3.2Wall Pressure Wavenumber-Frequency Spectrum 278 3.3Coreos' Similarity Model 280 3.3.1 Wavenumber/Phase-Velocity Spectrum 287 3.3.2Discussion on the Linearizing Assumption 288 3.4Landahi's Wave-Guide Model 288 3.5Shubert & Coreos' Linear Model 292 3.6Ffowcs Williams' Extension of Coreos' Model 297 3.7Chase's Wall Pressure Spectrum Model 307 4Gust-Response Aerodynamic Theories 317 4.1Introduction 317 4.2Possio's Integral Equation 318 4.3Sears' Gust-Response Solution 319 4.4Filotas' Model of Oblique Gust-Airfoil Interaction 323 4.5Amiet's Theory of Low- and High-Frequency Unsteady Flow Pasta Thin Airfoil .
Recommended publications
  • Numerical Buckling Analysis of Hybrid Honeycomb Cores for Advanced Helmholtz Resonator Liners
    Article Numerical Buckling Analysis of Hybrid Honeycomb Cores for Advanced Helmholtz Resonator Liners Moritz Neubauer , Martin Dannemann * , Michael Kucher , Niklas Bleil, Tino Wollmann and Niels Modler Institute of Lightweight Engineering and Polymer Technology (ILK), Technische Universität Dresden, Holbeinstraße 3, 01307 Dresden, Germany; [email protected] (M.N.); [email protected] (M.K.); [email protected] (N.B.); [email protected] (T.W.); [email protected] (N.M.) * Correspondence: [email protected]; Tel.: +49-351-463-38134 Abstract: In order to realize novel acoustic liners, honeycomb core structures specially adapted to these applications are required. For this purpose, various design concepts were developed to create a hybrid cell core by combining flexible wall areas based on thermoplastic elastomer films and rigid honeycomb areas made of fiber-reinforced thermoplastics. Within the scope of the presented study, a numerical approach was introduced to analyze the global compressive failure of the hybrid composite core structure, considering local buckling and composite failure according to Puck and Cuntze. Therefore, different geometrical configurations of fiber-reinforced tapes were compared with respect to their deformation as well as their resulting failure behavior by means of a finite element analysis. The resulting compression strength obtained by a linear buckling analysis agrees largely with calculated strengths of the more elaborate application of the failure criteria according to Puck and Cuntze, which were implemented in the framework of a nonlinear buckling analysis. Citation: Neubauer, M.; The findings of this study serve as a starting point for the realization of the manufacturing concept, Dannemann, M.; Kucher, M.; Bleil, N.; for the design of experimental tests of hybrid composite honeycomb core structures, and for further Wollmann, T.; Modler, N.
    [Show full text]
  • Development of a Fully-Coupled Harmonic Balance Method and A
    Development of a Fully-Coupled Harmonic Balance Method and a Refined Energy Method for the Computation of Flutter-Induced Limit Cycle Oscillations of Bladed Disks with Nonlinear Friction Contacts Christian Bertholdb, Johann Grossa, Christian Freyb, Malte Kracka aInstitute of Aircraft Propulsion Systems, University of Stuttgart, Pfaffenwaldring 6, 70569 Stuttgart, Germany [email protected], [email protected] bInstitute of Propulsion Technology, German Aerospace Center, Linder Höhe, 51147 Cologne, Germany [email protected], [email protected] Abstract Flutter stability is a dominant design constraint of modern gas and steam turbines. To further increase the feasible design space, flutter-tolerant designs are currently explored, which may undergo Limit Cycle Oscillations (LCOs) of acceptable, yet not vanishing, level. Bounded self-excited oscillations are a priori a nonlinear phenomenon, and can thus only be explained by nonlinear interactions such as dry stick-slip friction in mechanical joints. The currently available simulation methods for blade flutter account for nonlinear interactions, at most, in only one domain, the structure or the fluid, and assume the behavior in the other domain as linear. In this work, we develop a fully-coupled nonlinear frequency domain method which is capable of resolving nonlinear flow and structural effects. We demonstrate the computational performance of this method for a state-of-the-art aeroelastic model of a shrouded turbine blade row. Besides simulating limit cycles, we predict, for the first time, the phenomenon of nonlinear instability, i.e. , a situation where the equilibrium point is locally stable, but for sufficiently strong perturbation (caused e.g.
    [Show full text]
  • Application of the Bernoulli Enthalpy Concept to the Study of Vortex ‘Noise and Jet Impingement Noise
    NASA Contractor Report 2987 Application of the Bernoulli Enthalpy Concept to the Study of Vortex ‘Noise and Jet Impingement Noise John E. Yates CONTRACT NASJ-14503 APRIL 1978 - I TECH LIBRARY KAFB, NM NASA Contractor Report 2987 Application of the Bernoulli Enthalpy Concept to the Study of Vortex Noise and Jet Impingement Noise John E. Yates Aeromuticd Research Associates of Pritlceton, Ix. Primeton, New Jersey Prepared for Langley Research Center under Contract NASI-14503 National Aeronautics and Space Administration Scientific and Technical Information Office 1978 -- - TABLE OF CONTENTS SUMMARY 1 I. INTRODUCTION 2 Nomenclature 3 II. ACOUSTIC THEORY OF HOMENTROPIC FLOWS A. Assumptions and Basic Equations B. A Kinematic Definition of Sound L4 C. Acoustic Theory 11 D. Energy Theorem 14 E. The Kinetic Origin of Sound - The Liepmann Analogy 15 F. How is Sound Processed by a Fluid Flow? 18 G. How Does Sound Affect a Fluid Flow? 20 H. Comparison with Other Theories 20 III. INTERACTION OF SOUND WITH STEADY VORTEX FLOWS A. Plane Wave Scattering by a Vortex with Core Structure 24 B. Acoustic Interaction with Discrete Weakly Interacting Vortices C. Line Source Interaction with a ‘,ine Vortex D. Scattering of Engine Noise by an Aircraft Vortex Wake IV. PRODUCTION OF SOUND BY VORTEX FLOWS A. The Corotating Vortex Pair 48 B. Jet Impingement Noise C. A Suggested Problem 2: V. EXCITATION OF A FLUID FLOW BY SOUND A. Discussion of Experimental Results B. The Liepmann Analogy Revisited 2 C. Excitation of the Corotating Vortex Pair 62 D. Qualitative Comparison with Experiment 69 VI. CONCLUSIONS 76 REFERENCES iii John E.
    [Show full text]
  • Aeroacoustics of Space Vehicles
    National Aeronautics and Space Administration Aeroacoustics of Space Vehicles Jayanta Panda NASA Ames Research Center Moffett Field, CA Presentation for Applied Modeling & Simulation (AMS) Seminar Series Building N258, Auditorium (Room 127), NASA Ames Research Center Moffett Field, CA April 8, 2014 1 Jay Panda (NASA ARC) 4/7/2014 National Aeronautics and Space Administration Introduction ● Definition Aeroacoustics ●Aeroacoustics for Airplanes Mostly for community noise reduction very few vibro-acoustics concerns (such as failures of nozzle cowlings) ● Aeroacoustics for space vehicles Mostly for vibro-acoustic concern Intense vibrational environment for payload, electronics and navigational equipment and a large number of subsystems Community noise - little concern until recent time Environment inside ISS– separate issue ____Jay Panda (NASA ARC) 4/8/2014 2 National Aeronautics and Space Administration Introduction 185 Inside flame trench Typical levels (dB) of surface pressure 180 Shock-plume interaction fluctuations on launch vehicles Pad/low altitude abort Transonic Oscillating shock High altitude abort ? 170 AbortAcoustics Base of Vehicle Protuberances, Separated flow regions 160 20dB = X10 40dB = X100 60dB =X1000 Ascent AcousticsAscent 150 Launch AcousticsLaunch Smooth parts of vehicle 140 Tip of Vehicle Level inside cargo compt, payload fairing 130 Threshold of ear pain 120 dB Max Level inside Crew cabin 115 Loud Rock Concert ____Jay Panda (NASA ARC) 4/7/2014 3 National Aeronautics and Space Administration Introduction The end
    [Show full text]
  • Aerodynamic Analysis of the Undertray of Formula 1
    Treball de Fi de Grau Grau en Enginyeria en Tecnologies Industrials Aerodynamic analysis of the undertray of Formula 1 MEMORY Autor: Alberto Gómez Blázquez Director: Enric Trillas Gay Convocatòria: Juny 2016 Escola Tècnica Superior d’Enginyeria Industrial de Barcelona Aerodynamic analysis of the undertray of Formula 1 INDEX SUMMARY ................................................................................................................................... 2 GLOSSARY .................................................................................................................................... 3 1. INTRODUCTION .................................................................................................................... 4 1.1 PROJECT ORIGIN ................................................................................................................................ 4 1.2 PROJECT OBJECTIVES .......................................................................................................................... 4 1.3 SCOPE OF THE PROJECT ....................................................................................................................... 5 2. PREVIOUS HISTORY .............................................................................................................. 6 2.1 SINGLE-SEATER COMPONENTS OF FORMULA 1 ........................................................................................ 6 2.1.1 Front wing [3] .......................................................................................................................
    [Show full text]
  • An Introduction to Aeroacoustics
    An introduction to aeroacoustics A. Hirschberg∗ and S.W. Rienstra∗∗ Eindhoven University of Technology, ∗Dept. of App. Physics and ∗∗Dept. of Mathematics and Comp. Science, P.O. Box 513, 5600 MB Eindhoven, The Netherlands. Email: [email protected] and [email protected] 18 Jul 2004 20:23 18 Jul 2004 1 version: 18-07-2004 1 Introduction Due to the nonlinearity of the governing equations it is very difficult to predict the sound production of fluid flows. This sound production occurs typically at high speed flows, for which nonlinear inertial terms in the equation of motion are much larger than the viscous terms (high Reynolds numbers). As sound production represents only a very minute fraction of the energy in the flow the direct prediction of sound generation is very difficult. This is particularly dramatic in free space and at low subsonic speeds. The fact that the sound field is in some sense a small perturbation of the flow, can, however, be used to obtain approximate solutions. Aero-acoustics provides such approximations and at the same time a definition of the acoustical field as an extrapolation of an ideal reference flow. The difference between the actual flow and the reference flow is identified as a source of sound. This idea was introduced by Lighthill [68, 69] who called this an analogy. A second key idea of Lighthill [69] is the use of integral equations as a formal solution. The sound field is obtained as a convolution of the Green’s function and the sound source. The Green’s function is the linear response of the reference flow, used to define the acoustical field, to an impulsive point source.
    [Show full text]
  • Computational Aeroacoustics: Progress on Nonlinear Problems of Soundgeneration Tim Coloniusa,Ã, Sanjiva K
    ARTICLE IN PRESS Progress in Aerospace Sciences 40 (2004) 345–416 Computational aeroacoustics: progress on nonlinear problems of soundgeneration Tim Coloniusa,Ã, Sanjiva K. Leleb aDepartment of Mechanical Engineering, California Institute of Technology, Mail Code 104-44 Pasadena, CA 91125, USA bDepartment of Aeronautics and Astronautics and Department of Mechanical Engineering, Stanford University, Stanford, CA 94305-4035, USA Abstract Computational approaches are being developed to study a range of problems in aeroacoustics. These aeroacoustic problems may be classifiedbasedon the physical processes responsible for the soundradiation,andrange from linear problems of radiation, refraction, and scattering in known base flows or by solid bodies, to sound generation by turbulence. In this article, we focus mainly on the challenges andsuccesses associatedwith numerically simulating soundgeneration by turbulent flows. We discuss a hierarchy of computational approaches that range from semi-empirical schemes that estimate the noise sources using mean-flow and turbulence statistics, to high-fidelity unsteady flow simulations that resolve the sound generation process by direct application of the fundamental conservation principles. We stress that high-fidelity methods such as Direct Numerical Simulation (DNS) and Large Eddy Simulation (LES) have their merits in helping to unravel the flow physics and the mechanisms of sound generation. They also provide rich databases for modeling activities that will ultimately be needed to improve existing predictive capabilities. Spatial and temporal discretization schemes that are well-suited for aeroacoustic calculations are analyzed, including the effects of artificial dispersion and dissipation on uniform and nonuniform grids. We stress the importance of the resolving power of the discretization as well as computational efficiency of the overall scheme.
    [Show full text]
  • Linearized Navier-Stokes Solver for In-Duct Aeroacoustics
    Linearized Navier-Stokes solver for in-duct aeroacoustics GUNILLA EFRAIMSSON Department of Aeronautical and Vehicle Engineering KTH, Stockholm, Sweden [email protected] Axel Kierkegaard, Wei Na, Mats Åbom, Ciarán O’Reilly, Susann Boij, Hans Bodén Outline • Tango-aspects • Linearized Navier-Stokes equations solver • Two tecases - Area expansion - Thick orifice • Conclusions and future work Tango setting Q˙ 0 Unsteady heat release Generation of sound waves Perturbation flow & flame Pressure Oscillation p0 Study the coupling sound , flow and heat release using linearized Navier-Stokes equations Generation and Propagation of Sound • Generation Fans, rotor-stator interaction, constrictions, jets, combustion - Acoustic analogies, direct methods - Transient phenomena è transient simulations (LES,, DES, uRANS) or scaling laws • Propagation Free air, pipes, influence of flow, influence of solid surfaces (shielding), coupling of sound and flow (whistling, damping of sound), duct terminations - Linear equations in time or frequency domain: Helmholtz equation, wave equation, linearized Euler equations etc Propagation of sound in ducts with constrictions Straight cylindrical duct with orifice plate Turbulent meanflow Incoming waves are partly reflected and partly transmitted Reflections from downstream obstacles (or boundary conditions) Zone I Zone III Zone IV Zone II x 0 1 = x2 = 0 Propagation of sound in ducts with constrictions Straight cylindrical duct with orifice plate Turbulent meanflow Incoming waves are partly reflected and partly transmitted Reflections
    [Show full text]
  • Aerodynamics and Aeroacoustics of a Vertical Axis Wind Turbine
    15th EAWE PhD Seminar on Wind Energy 29-31 October 2019 Ecole Centrale de Nantes, France Aerodynamics and aeroacoustics of a Vertical Axis Wind Turbine L Brandettia, F Avallonea, C J Simao Ferreiraa, D Casalinoa a AWEP Dept., Faculty of Aerospace Engineering, Delft University of Technology, Delft, the Netherlands E-mail: [email protected] Keywords: Vertical Axis Wind Turbine, Aeroacoustics, Aerodynamics. According to the orientation of the axis of rotation, wind turbines are classified in: Horizontal Axis Wind Turbines (HAWTs) and Vertical Axis Wind Turbines (VAWTs). Next to the most conventional and economically feasible HAWTs, VAWTs have advantages: the intrinsic omnidirectionality of VAWTs does not require the design of yaw motors; the location of the generator on the ground leads to easier access and, consequently, lower maintenance cost [1]; they are visually more appealing and suitable for the installation into urban environments. In order to be located in an urban environment, noise regulations must be respected. For operating wind turbines, it is possible to distinguish between mechanical and aerodynamic noise sources. The first one is caused by the dynamic response of the moving mechanical components while the latter is produced by the interaction of the airflow with the blades [2]. Nowadays, the major focus is on aerodynamic noise, proving that mechanical noise has been already optimized [3]. Aerodynamic noise can be divided in: turbulent-impingement (T-I) noise and airfoil-self noise. T-I noise occurs when the incoming turbulence interacts with the blade leading edge [4][5]. In literature, there is no agreement on how to model it.
    [Show full text]
  • Fundamentals of Fan Aeroacoustics Overview of Lecture
    Fundamentals of Fan Aeroacoustics Overview of Lecture • Noise Sources and Generation Mechanisms – Sources of Noise for Typical Fans – Fluid-Structure Interaction as a Noise Generation Mechanism – Coupling to the Duct: Propagating Modes and Cut-off Phenomena • Modeling of Fan Noise The Acoustic Analogy Computational Methods:Aeroacoustics and UnsteadyAerodynamics The Linear Cascade Model Effects of Geometry and Blade Loading on Acoustic Radiation • Recent Developments in Fan Modeling – Tonal and Broadband Noise – Nonuniform Mean Flow Effects:swirl – Three-Dimensional Effects – High Frequency Effects • Conclusions Dominant Noise Sources for Turbofan Engines High Bypass Ratio Fan Flyover Noise Maximum Perceived Noise Level Approach Takeoff Typical Turbomachinery Sound Power Spectra Subsonic Tip Speed Supersonic Tip Speed Turbomachinery Noise Generation Process Rotor-Stator Interaction Fluid-Structure Interaction as a Noise Generation Mechanism • The interaction of nonuniform flows with structural components such as blades and guide vanes produce fluctuating aerodynamic forces on the blades and radiates sound in the farfield. • Noise Sources: Flow Nonuniformities: Inlet Turbulence, Boundary Layers, Tip and Hub Vortices,Wakes etc. • Mechanism: Interaction with Rotating Components (rotor noise), Scattering by Sharp Edges (trailing edge noise), Impingement of Unsteady Nonuniformities on Guide Vanes (rotor/stator interaction). • Propagation in the Duct: Sound Must Propagate in a Duct: therefore only high frequency acoustic modes will propagate.
    [Show full text]
  • Surface Integral Methods in Computational Aeroacoustics
    Surface Integral Metho ds in Computational Aeroacoustics -From the CFD Near-Field to the Acoustic Far-Field y Anastasios S. Lyrintzis Scho ol of Aeronautics and Astronautics Purdue University W. Lafayette, IN 47907-2023 Abstract A review of recent advances in the use of integral metho ds in Computational AeroAcoustics CAA for the extension of near- eld CFD results to the acoustic far- eld is given. These integral formulations i.e. Kirchho 's metho d, p ermeable p orous surface Ffowcs-Williams Hawkings FW-H equation allow the radiating sound to b e evaluated based on quantities on an arbitrary control surface if the wave equation is assumed outside. Thus only surface integrals are needed for the calculation of the far- eld sound, instead of the volume integrals required by the traditional acoustic analogy metho d i.e. Lighthill, rigid b o dy FW-H equa- tion. A numerical CFD metho d is used for the evaluation of the ow- eld solution in the Presented at the CEAS Workshop \From CFD to CAA" Athens Greece, Nov. 2002. y Professor, e-mail: [email protected]. 1 near eld and thus on the control surface. Di usion and disp ersion errors asso ciated with wave propagation in the far- eld are avoided. The surface integrals and the rst derivatives needed can b e easily evaluated from the near- eld CFD data. Both metho ds can b e ex- tended in order to include refraction e ects outside the control surface. The metho ds have b een applied to helicopter noise, jet noise, prop eller noise, ducted fan noise, etc.
    [Show full text]
  • Interdependence of Friction, Wear, and Noise: a Review
    Friction 9(6): 1319–1345 (2021) ISSN 2223-7690 https://doi.org/10.1007/s40544-021-0500-x CN 10-1237/TH REVIEW ARTICLE Interdependence of friction, wear, and noise: A review Kevin LONTIN*, Muhammad KHAN Cranfield University, MK43 0AL, UK Received: 02 July 2020 / Revised: 02 November 2020 / Accepted: 29 January 2021 © The author(s) 2021. Abstract: Phenomena of friction, wear, and noise in mechanical contacts are particularly important in the field of tribomechanics but equally complex if one wants to represent their exact relationship with mathematical models. Efforts have been made to describe these phenomena with different approaches in past. These efforts have been compiled in different reviews but most of them treated friction, wear mechanics, and acoustic noise separately. However, an in-depth review that provides a critical analysis on their interdependencies is still missing. In this review paper, the interdependencies of friction, wear, and noise are analysed in the mechanical contacts at asperitical level. The origin of frictional noise, its dependencies on contact’s mechanical properties, and its performance under different wear conditions are critically reviewed. A discussion on the existing mathematical models of friction and wear is also provided in the last section that leads to uncover the gap in the existing literature. This review concludes that still a comprehensive analytical modelling approach is required to relate the interdependencies of friction, noise, and wear with mathematical expressions. Keywords: noise; acoustic emission; wear; friction 1 Introduction computations using only the dominant harmonic components as opposed to full harmonic components Wear processes present a severe challenge in industry.
    [Show full text]