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nanosecond dielectric barrier discharge plasma actuator PDF

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Preview nanosecond dielectric barrier discharge plasma actuator

NANOSECOND DIELECTRIC BARRIER DISCHARGE PLASMA ACTUATOR CHARACTERIZATION AND APPLICATION NANOSECOND DIELECTRIC BARRIER DISCHARGE PLASMA ACTUATOR CHARACTERIZATION AND APPLICATION Proefschrift terverkrijgingvandegraadvandoctor aandeTechnischeUniversiteitDelft, opgezagvandeRectorMagnificusprof.ir.K.C.A.M.Luyben, voorzittervanhetCollegevoorPromoties, inhetopenbaarteverdedigenopMaandag8februari2016om10:00uur door GiuseppeCORREALE MasterofScienceinAerospaceEngineering DelftUniversityofTechnology,TheNetherlands geborenteNapels,Italië. Ditproefschriftisgoedgekeurddoordepromotor: Prof.dr.F.Scarano Copromotor:Dr.M.Kotsonis Samenstellingpromotiecommissie: RectorMagnificus, voorzitter Prof.dr.F.Scarano, TechnischeUniversiteitDelft,promotor Dr.M.Kotsonis, TechnischeUniversiteitDelft,copromotor Independentmembers: Prof.dr.ir.L.L.M.Veldhuis, TechnischeUniversiteitDelft Prof.dr.J.Little, ArizonaStateUniversity,US Prof.dr.J.P.Bonnet, UniversitedePoitiers,FR Dr.P.Leyland, EcolePolytechniqueFederaledeLausanne,CH Prof.dr.N.Benard, UniversitedePoitiers,FR Prof.dr.ir.G.vanBussel, TechnischeUniversiteitDelft,reservelid v Keywords: ns-DBDPlasmaActuator Printedby: IpskampDrukkers Front&Back: WheatfieldwithCrows,VincentVanGogh Graphicby: Copyright©2016byGiuseppeCorreale ISBN978-94-6186-603-5 Anelectronicversionofthisdissertationisavailableat http://repository.tudelft.nl/. Autviaminveniamautfaciam. Annibale Ishalleitherfindawayeithermakeone. Hannibal S UMMARY AN experimental investigation about nanosecond Dielectric Barrier Discharge (ns- DBD)plasmaactuatorispresentedinthisthesis. Thisworkaimedtoanswerfun- damentalquestionsontheactuationmechanismofthisdevice. Inordertodoso,para- metric studies in a quiescent airas wellaslaminar bounded offreeshear layerswere performed. Amplitudeandlocationoftheinputwithrespecttothereceptivity region as well as frequency of flow actuation were investigated. This work required the im- plementation of acquisition techniques such as Schlieren, Particle Image Velocimetry (PIV),infraredthermography,backcurrentshunttechniqueandbalancemeasurements. Moreover,toolsofanalysiswereemployedsuchasLinearStabilityTheory(LST),Proper OrthogonalDecomposition(POD)andInverseHeatTransferProblem(IHTP). Resultsrevealedthattheeffectofans-DBDisthatof“enhancing”thedevelopment ofnaturalhydrodynamicinstabilitiesofthespecificfieldofmotion. Therefore,incase of a laminar boundary layer, the effect of a ns-DBD plasma actuator was to amplify Tollmien–Schlichting wavesaccordingtolinearstabilitytheory. Suchresultsledtoun- derstand the influence of the actuator position on the achievement of a specific flow controltask. Ans-DBDiscapableofproducingseveraleffects: ashockwave,asmallbodyforce and a thermal gradient within the discharge volume. Thus, three were the possible causes of flowactuation. The shock wavewasfound to betoo weakto becapable of introducinganappreciabledisturbance. Astheshockwave,alsothemomentuminjec- tioninducedbythebodyforceproducedbythepulseddischargewasfoundtoberela- tivelytoosmalltojustifyacontrolauthoritybasedonmomentumredistributionwithin the boundary layer, for cases of relatively high freestream velocity. Thus, the thermal gradientinducedwithinthedischargevolumebytheenergydepositionofahighvolt- agenanoseconddischargeistheeffectcapableofinducingarelativelylargedisturbance intothefieldofmotion.Nevertheless,athermalgradientwithinagaseousflowinduces twoeffects, itreducesdensityandincreasesviscosity. Atthemomentitisstillunclear whichofthesetwoeffectsismorerelevant. Onceidentifiedthethermalgradientasthe maincauseofflowcontrolmechanism,acharacterizationstudywasperformedaimed toidentifythepropertiesofans-DBDplasmaactuator(thermal,electricalandgeomet- rical)importanttomaximizetheinducedthermalgradientwithinthedischargevolume. Ingeneral,ahigherefficiencyisachievedbyastrongdielectricmaterialconcerning thermalenergydeposition. Abarrierofans-DBDplasmaactuatorshouldbeasthinas possible.However,thethicknessaffectsalsothelifetimeofthebarrieritself. NanosecondpulsedDBDplasmaactuatorshaveshowntohavethecapabilitytode- layleadingedgeseparation. However,intherelevantliterature,aninfluenceoftheac- tuationfrequencyontheachievedresultsisalwaysreported.Inordertoinvestigatethis frequency effect, a parametric study ona BackwardFacing Step wasperformed. This geometrywasselectedbecauseitmimicsafixedpointlaminarseparation,theflowsce- ix x SUMMARY narioofinterest.Suchflowscenarioisunstableathighfrequenciesclosetothestepand lowfrequencies downstreamthestepanditnaturally developsamostunstable mode withinit. However,whenaflowisactuated,itsstabilitychanges,sodothemostunsta- blefrequenciesnaturallydevelopedwithinit.Resultsshowedthattheeffectofactuation istheredistributionofenergyamongmodesandthattheoptimalfrequencyofactua- tionmustbebasedonthenewstabilityachievedbytheflowduetotheactuationitself. Moreover,resultsindicatedthattheoptimalfrequencyofactuationisnotrelatedtothe mostunstablefrequenciesnaturallypresentwithinthebasenon-actuatedflow. Amethodtoquantifytheefficiencyofns-DBDsindepositingenergywithinthedis- chargevolume is proposed. This energy is the one that eventually contributes to the formationofthethermalgradientresponsibleoftheflowcontrolcapabilitiesshownby thesedevices. Suchmethodisbasedonsimultaneousimplementationofinfraredther- mographyandback-currentshunttechniques.Resultsshowedthattheoverallefficiency ofans-DBDplasmaactuatorisinverselyproportionaltothethicknessofthedielectric barrier. Lastpartofthisthesisisconcernedwithademonstrative applicationofans-DBD plasmaactuatoronatwoelementairfoil,atReynoldsnumbersrangingbetween0.2 106 · and2 106. Resultsdemonstrateditscapabilitytodelayseparation,increaseliftandre- · ducedraginthepoststallregime.Moreover,theplasmaactuatorshowedthecapability toeliminatebothalaminarbubbleseparationforsmallanglesofattackandthehystere- sisbehaviouroftheselectedairfoil. Inconclusion,thisworkshedsomelightontheflowactuationmechanismofans- DBDplasmaactuatoranddeepeneditsbasicknowledge.

Description:
NANOSECOND DIELECTRIC BARRIER DISCHARGE A barrier of a ns-DBD plasma actuator should be as thin as possible defined in equation 1.9 as the ratio between the local flow velocity (U) and the local boundary layer developing on the curved surface of an airfoil, as illustrated in figure 1.3.
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