Abstract

Abstract The influence of Stokes number on the evolution ofthe distributions of particle concentration and velocityfrom their exit values is reported for a co-flowing jetissuing from a long pipe. The data are obtained bysimultaneous Planar Nephelometry and Particle ImageVelocimetry using four cameras to provide high resolu-tionthroughthefirst30jetdiametersandalsocorrectionforopticalattenuation. Thesedataprovidemuchmoredetailedinformationthanisavailablefrompreviousmea-surements. TheseprovidenewunderstandingofhowtheStokes number influences the flow at the jet exit planeandhowthisinfluencepropagatesthroughoutthejet. 1. INTRODUCTION Particle-laden turbulent jets, typically consisting ofsolidparticlessuspendedinaconveyingfluid,areanim-portantclassofflow,notonlybecauseoftheirfundamen-talsignificance,butalsobecauseoftheirwiderelevancetomanyapplicationssuchasintheflamesofboilersandfurnaces. Thecombustionintheseprocessestypicallyoc-cursintheturbulentregime,sothatparticle-flowinter-actionsinfluencethedistributionsofbothresidencetimeandstoichiometry. Hencetheyalsoinfluencethein-flamedistributionsoftemperatureandspeciesconcentrations,which in turn influence the key performance character-isticsoftheflamedimensions,radiantheattransferandpollutant emissions [1]. Therefore, an understanding ofparticle-laden flows is crucial to optimising combustionprocesses in industrial systems to enable the design ofsafer,moreenergyefficientcombustionwithloweremis-sions. Thesignificanceoftheseflowshasresultedincon-siderableefforttounderstandthemovertheyears,withtheresultthatmuchisnowknownaboutparticle-ladenturbulent jets [2–12]. However, the greater complexityoftheseflowsovertheirsingle-phasecounterpart,whichincludestheintroductionofmanyadditionalparameterstogether with the many additional experimental chal-lenges introduced both by the conveying fluid and themeasurement of particle-laden flows, means that manygaps in understanding persist. The overall aim of thepresentinvestigationistomeetthisneedthroughade-tailedandsystematicexperimentalinvestigationofwell-characterisedturbulent,particle-ladenjets.Thefullcharacterisationofparticle-ladenturbulentjets requires the simultaneous measurement of the ve-locity field of both phases, together with the local, in-stantaneousparticlesizeandnumberdensity. Preferablysuchmeasurementsshouldalsobeperformedsimultane-ously in multiple dimensions and with sufficient spatialand temporal resolution owing to the turbulent natureof the flow. This challenge is so great that previousexperiments of particle-laden jets have each performedonly limited measurements that provide incomplete de-tail of the flow and/or address only a small number offlow conditions. Additionally, the different experimentsperformed in each laboratory have all been performedwith different initial and/or boundary conditions, suchas particle size distribution, particle mass loading andnozzlegeometry. Furthermore,nopreviousinvestigationhas provided a complete description of the inflow con-ditions, such as detailed profiles of the mean and fluc-tuating components of the velocity and scalar fields atthe nozzle exit. Hence there is a need for detailed andcomprehensive measurements of the velocity and scalarfieldsofturbulentjetsspanningawiderangeofcontrolvariables,suchastheStokesnumber.Previous measurements of the velocity and scalarfields of particle-laden turbulent jets are shown in Ta-ble1. Ofthepreviousmeasurementsofthevelocityfield[2–12], only five [8–12] also report the concentration ofthedispersedphase. Ofthese,nonereporttheimportantStokesnumber(

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