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Understanding and controlling vorticity transport in unsteady, separated flows PDF

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University of Iowa Iowa Research Online Theses and Dissertations Fall 2015 Understanding and controlling vorticity transport in unsteady, separated flows James Akkala University of Iowa Copyright 2015 James Akkala This dissertation is available at Iowa Research Online: https://ir.uiowa.edu/etd/1947 Recommended Citation Akkala, James. "Understanding and controlling vorticity transport in unsteady, separated flows." PhD (Doctor of Philosophy) thesis, University of Iowa, 2015. https://doi.org/10.17077/etd.8t9jvlnt Follow this and additional works at:https://ir.uiowa.edu/etd Part of theMechanical Engineering Commons UNDERSTANDINGANDCONTROLLINGVORTICITYTRANSPORTIN UNSTEADY,SEPARATEDFLOWS by JamesAkkala Athesissubmittedinpartialfulfillmentofthe requirementsfortheDoctorofPhilosophy degreeinMechanicalEngineering intheGraduateCollegeof TheUniversityofIowa December2015 ThesisSupervisor: JamesH.J.Buchholz GraduateCollege TheUniversityofIowa IowaCity,Iowa CERTIFICATEOFAPPROVAL PH.D.THESIS ThisistocertifythatthePh.D.thesisof JamesAkkala has been approved by the Examining Committee for the thesis requirement for the Doctor ofPhilosophydegreeinMechanicalEngineeringattheDecember2015graduation. ThesisCommittee: JamesH.J.Buchholz,ThesisSupervisor ChristophBeckermann DonaldGurnett Ching-longLin FrederickStern ACKNOWLEDGEMENTS I would like to begin by thanking Professor James Buchholz for the tremendous encouragement,guidanceandsupportthathehasprovidedtomethroughoutthisendeavor. Without his inspiration, optimism and confidence in my abilities, this work could not have been accomplished. I would also like to thank him for affording me the privilege of par- ticipating in the Air Force Summer Faculty Fellowship Program and for giving me the opportunitytopresentmyworkatseveralconferences. Iwouldalsoliketothankmyesteemedcommitteemembers,Prof. ChristophBeck- ermann, Prof. Donald Gurnett, Prof. Ching-Long Lin and Prof. Frederick Stern for their valuabletime andinsightful discussion. My sincerethanks alsoextends tomyclose friend KatieRadtkeforgenerouslyservingasmythesisreaderandprovidinginvaluablefeedback forimprovingthequalityofthiswork. It has been my pleasure to work with an amazing research team at the University of Iowa. Azar Eslam Panah, Kevin Wabick and Craig Wojcik, in particular, have been outstandingco-collaboratorsandIamfortunatetohavehadthechancetoworkwiththem. Lastbutnotleast,Iwanttothankmyparentsfortheirsteadfast supportinallthatI do, as well as my friends at the University of Iowa for providing me with some of the best timesofmylife. This work was supported in part by the Air Force Office of Scientific Research, awardnumberFA9550-11-1-0019,andbyIIHR-Hydroscience&Engineering. ii ABSTRACT Vortices interacting with the solid surface of aerodynamic bodies are prevalent across a broad range of geometries and applications, such as dynamic stall on wind tur- bine and helicopter rotors, the separated flows over flapping wings of insects, birds and micro-air vehicles, formation of the vortex wakes of bluff bodies, and the lift-producing vortices formed by aircraft leading-edge extensions and delta wings. This study provides fundamental insights into the formation and evolution of such vortices by considering the leading-edgevorticesformedinvariationsofacanonicalflappingwingproblem. Specifically, the vorticity transport within three distinct experimental cases–2D plunging airfoil, 3D plunging airfoil and 2D plunging airfoil with suction applied at the leading edge–were analyzed in order to characterize the formation and evolution of the leading-edgevortex(LEV). Three-dimensionalrepresentationsofthevelocityandvorticityfieldswereobtained via multi-plane particle image velocimetry (PIV) measurements and used to perform a vorticity flux analysis that served to identify the sources and sinks of vorticity within the flow. Time-resolved pressure measurements were obtained from the surface of the airfoil andusedtocharacterizethefluxofvorticitydiffusingfromthesolidsurface,andamethod forcorrectingdynamicpressuredatawasdevelopedandvalidatedfortheapplicationwithin thecurrentstudy. Upon characterizing all of the sources and sinks of vorticity, the circulation budget wasfoundtobefullyaccountedfor. Interpretationoftheindividualvorticitybalanceterms iii demonstrated vorticity generation and transport characteristics that were consistent among all three cases that were investigated. Three-dimensional vorticity fluxes were found to be an almost negligible contributor to the overall circulation budget, mostly due to the individual terms canceling each other out. In all cases, the diffusive flux of vorticity from the surface of the airfoil was shown to act primarily as a sink of LEV vorticity, with a magnitude roughly half that of the flux of vorticity emanating from the leading-edge shear layer. Inspection of the chordwise distribution of the diffusive flux within the 2D case showed it to correlate very well with the evolution of the flow field. Specifically, the diffusive flux experienced a major increase during the phase interval in which the LEV remained attached to the downstream boundary layer. It was also noted that the accu- mulation of secondary vorticity near the leading edge prevented the diffusive flux from continuingtoincreaseaftertheroll-upoftheLEV.Thisresultwasvalidatedwithinthe3D case, which demonstrated that maintaining an LEV that stays attached to the downstream boundarylayerproducesalargerdiffusivefluxofvorticity–presumablyenhancingbothlift andthrust. Through the use of a spanwise array of suction ports, the suction case was able to successfully alter the total circulation of the flow by removing positive vorticity from the opposite-signed vortex (OSV) that formed beneath the LEV. This removal of positive vorticityproducedameasuredincreaseinthetotallift,anditwasnotedthatweakeningthis region of secondary vorticity allowed the LEV to impose more suction on the surface of the airfoil. However, it was also noted that weakening the OSV resulted in a loss of thrust, iv which was attributed to the loss of suction that occurred near the leading edge when the removal of secondary vorticity caused the energetic OSV to be reverted into a low energy regionofseparatedflow. Thephysicalinsightsprovidedbythisworkcanformthebasisofnovelflowcontrol strategiesforenhancingtheaerodynamicloadsproducedinunsteady,separatedflows. v PUBLICABSTRACT The interaction between vortices and the solid surface of an aerodynamic body is a ubiquitous feature of high-angle-of-attack aerodynamics associated with a broad range of aerospace structures, including maneuvering and flapping wings, blades on helicopter ro- torsandgasturbineengines,theaerodynamicforebodesofmissilesandhigh-performance aircraft. Thisstudyprovidesfundamentalinsightsintothedevelopmentofsuchvorticesby consideringthevortexformedattheleadingedgeofaplungingairfoil. The primary goal of this work was to rigorously characterize the formation and evolution of the leading-edge vortex (LEV) based on the transport of vorticity both within the bulk flow as well as near the surface of the airfoil. By performing a novel analysis thatservedtoquantifythenear-walldynamicsoftheflow,thisstudydemonstratedthatthe strength of the LEV was significantly reduced by its interaction with the solid surface. It was further shown that the near-wall vorticity transport mechanisms associated with this reduction also play a critical role in governing the formation and development of the LEV priortoitsdetachment. By explicitly characterizing how the vortex-airfoil interaction affects the evolution of the LEV, the results of this study have significantly enhanced our understanding of why the LEV develops the way it does. The physical insights provided by this work can form the basis of novel flow control strategies for enhancing the aerodynamic loads produced in unsteady,separatedflows. vi TABLEOFCONTENTS LISTOFTABLES . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . x LISTOFFIGURES . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . xi NOMENCLATURE . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . xix CHAPTER 1 INTRODUCTIONANDBACKGROUND . . . . . . . . . . . . . . . . . . 1 1.1 MotivationandGoals . . . . . . . . . . . . . . . . . . . . . . . . . . 1 1.2 LiteratureReview: TheLeading-EdgeVortex . . . . . . . . . . . . . . 2 1.2.1 LEVFormationProcess . . . . . . . . . . . . . . . . . . . . . 4 1.2.2 LEVScaling . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 1.2.3 EvolutionoftheLEV . . . . . . . . . . . . . . . . . . . . . . 9 1.2.4 EffectofCross-SectionalShapeofanAirfoil . . . . . . . . . . 14 1.2.5 Three-DimensionalVortexStructure . . . . . . . . . . . . . . 16 1.3 LiteratureReview: BoundaryVorticityDynamics . . . . . . . . . . . 19 1.3.1 VorticityTransportatBoundaries . . . . . . . . . . . . . . . . 20 1.3.2 FlowControlandBoundaryVorticityManipulation . . . . . . 30 1.4 Objective . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 33 1.5 Overview . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 2 DEVELOPMENTOFTHEVORTICITYFLUXANALYSIS . . . . . . . . 37 2.1 DerivationofVorticityFluxEquation . . . . . . . . . . . . . . . . . . 37 2.2 CharacterizationoftheDiffusiveFluxofVorticity . . . . . . . . . . . 43 2.3 ModelImplementation . . . . . . . . . . . . . . . . . . . . . . . . . . 50 3 METHODOLOGY . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 55 3.1 Overview . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 55 3.2 ModelGeometriesandExperimentalTechniques . . . . . . . . . . . . 56 3.3 Suction System and Internal Fluid Transmission Lines of the AR4 Airfoil . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 60 3.4 DigitalParticleImageVelocimetry . . . . . . . . . . . . . . . . . . . 70 3.4.1 StereoParticleImageVelocimetry: BaselineandSuctionCases 70 3.4.2 2DParticleImageVelocimetry: AR2Case . . . . . . . . . . . 76 3.5 ForceMeasurements . . . . . . . . . . . . . . . . . . . . . . . . . . . 78 3.6 TransientPressureMeasurements . . . . . . . . . . . . . . . . . . . . 80 vii 3.6.1 BaselineandSuctionCases . . . . . . . . . . . . . . . . . . . 80 3.6.2 Finite-ARCase . . . . . . . . . . . . . . . . . . . . . . . . . 82 3.6.3 PressureDataAcquisition . . . . . . . . . . . . . . . . . . . . 85 4 CORRECTIONOFDYNAMICPRESSUREMEASUREMENTS . . . . . . 86 4.1 Methods for Assessment and Correction of Transient Pressure Mea- surements . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 87 4.2 TestCase . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 91 4.3 DynamicCalibration . . . . . . . . . . . . . . . . . . . . . . . . . . . 91 4.4 InverseIdentificationMethods . . . . . . . . . . . . . . . . . . . . . 95 4.4.1 Validation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 98 4.5 ModelImplementationandCorrectionofPlungingAirfoilData . . . . 98 5 RESULTSFORTHEBASELINECASE . . . . . . . . . . . . . . . . . . . 100 5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 100 5.2 GlobalFlowDynamicsandLEVEvolution . . . . . . . . . . . . . . . 100 5.3 CharacterizationoftheVorticityBudget . . . . . . . . . . . . . . . . 103 5.3.1 Region A: AttachedFlow . . . . . . . . . . . . . . . . . . . . 113 5.3.2 Region B: SeparationattheLeadingEdge . . . . . . . . . . . 115 5.3.3 RegionC: LEVDetachment . . . . . . . . . . . . . . . . . . 118 5.3.4 Summary . . . . . . . . . . . . . . . . . . . . . . . . . . . . 120 6 CHARACTERIZATION OF THE FLOW PHYSICS GOVERNING THE FORMATIONOFTHELEV . . . . . . . . . . . . . . . . . . . . . . . . . 123 6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 123 6.2 FormationoftheLEV . . . . . . . . . . . . . . . . . . . . . . . . . . 123 6.3 DevelopmentoftheOSV . . . . . . . . . . . . . . . . . . . . . . . . 129 6.4 Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 132 7 FORCESONA2DPLUNGINGPLATE . . . . . . . . . . . . . . . . . . . 139 7.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 139 7.2 LiftDecomposition: ContributionsfromUpperandLowerSurfaces . . 142 7.3 LiftDecomposition: Viscous/InviscidContributions . . . . . . . . . . 146 7.4 AerodynamicsoftheLEV . . . . . . . . . . . . . . . . . . . . . . . . 149 7.5 OverviewofSubsequentChapters . . . . . . . . . . . . . . . . . . . . 154 8 RESULTSFORTHEFINITEASPECT-RATIOCASE . . . . . . . . . . . 155 8.1 GlobalFlowDynamicsandEvolution . . . . . . . . . . . . . . . . . . 155 8.2 FluxAnalysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 166 viii

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bine and helicopter rotors, the separated flows over flapping wings of insects, plunging airfoil, 3D plunging airfoil and 2D plunging airfoil with suction
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