Computational investigation of diesel nozzle internal flow during the complete injection event

[EN] Currently, diesel engines are calibrated using more and more complex multiple injection strategies. Under these conditions, the characteristics of the flow exiting the fuel injector are strongly affected by the transient interaction between the needle, the sac volume and the orifices, which are not yet clear. In the current paper, a methodology combining a 1D injector model and 3D-CFD simulations is proposed. First, the characteristics of the nozzle flow have been experimentally assessed in transient conditions by means of injection rate and momentum flux measurements. Later, the 3D-CFD modeling approach has been validated at steady-state fixed lift conditions. Finally, a previously developed 1D injector model has been used to extract the needle lift profiles and transient pressure boundary conditions used for the full-transient 3D-CFD simulations, using adaptive mesh refinement (AMR) strategies to be able to simulate the complete injection rate starting from 1 mu m lift.This work was partly sponsored by "Ministerio de Economia y Competitividad'', of the Spanish Government, in the frame of the Project "Estudio de la interaccion chorro-pared en condiciones realistas de motor'', Reference TRA2015-67679-c2-1-R. The authors would like also to thank the computer resources, technical expertise and assistance provided by Universidad de Valencia in the use of the supercomputer "Tirant''. Mr. Jaramillo's Thesis is funded by "Conselleria d'Educacio, Cultura i Esports'' of Generalitat Valenciana in the frame of the program "Programa VALI + D para investigadores en formacion, Reference ACIF/2015/040.Salvador, FJ.; De La Morena, J.; Bracho Leon, G.; Jaramillo-Císcar, D. (2018). Computational investigation of diesel nozzle internal flow during the complete injection event. Journal of the Brazilian Society of Mechanical Sciences and Engineering. 40(3):153-167. https://doi.org/10.1007/s40430-018-1074-zS153167403Hall CAS, Lambert JG, Balogh SB (2014) EROI of different fuels and the implications for society. Energy Policy 64:141–152. https://doi.org/10.1016/j.enpol.2013.05.049Lujan JM, Tormos B, Salvador FJ, Gargar K (2009) Comparative analysis of a DI diesel engine fuelled with biodiesel blends during the European MVEG-A cycle: preliminary study (I). Biomass Bioenergy 33:941–947. https://doi.org/10.1016/j.biombioe.2009.02.004Pickett LM, Siebers DL (2004) Soot in diesel fuel jets: effects of ambient temperature, ambient density, and injection pressure. Combust Flame 138:114–135. https://doi.org/10.1016/j.combustflame.2004.04.006Dec JE (1997) A Conceptual Model of DI Diesel Combustion Based on Laser-Sheet Imaging. SAE Tech. Pap. 970873Wang X, Huang Z, Zhang W et al (2011) Effects of ultra-high injection pressure and micro-hole nozzle on flame structure and soot formation of impinging diesel spray. Appl Energy 88:1620–1628. https://doi.org/10.1016/j.apenergy.2010.11.035Sayin C, Gumus M, Canakci M (2013) Influence of injector hole number on the performance and emissions of a di diesel engine fueled with biodiesel-diesel fuel blends. Appl Therm Eng 61:121–128. https://doi.org/10.1016/j.applthermaleng.2013.07.038Mohan B, Yang W, Chou SK (2013) Fuel injection strategies for performance improvement and emissions reduction in compression ignition engines—A review. Renew Sustain Energy Rev 28:664–676. https://doi.org/10.1016/j.rser.2013.08.051Payri R, Salvador FJ, Gimeno J, De la Morena J (2011) Influence of injector technology on injection and combustion development, Part 1: hydraulic characterization. Appl Energy 88:1068–1074. https://doi.org/10.1016/j.apenergy.2010.10.012Park SW, Kim JW, Lee CS (2006) Effect of injector type on fuel-air mixture formation of high-speed diesel sprays. Proc Inst Mech Eng D 220:647–659. https://doi.org/10.1243/09544070D20304Moon S, Komada K, Sato K et al (2015) Ultrafast X-ray study of multi-hole GDI injector sprays: effects of nozzle hole length and number on initial spray formation. Exp Therm Fluid Sci 68:68–81. https://doi.org/10.1016/j.expthermflusci.2015.03.027Powell CF, Kastengren AL, Liu Z, Fezzaa K (2010) The effects of diesel injector needle motion on spray structure. J Eng Gas Turbines Power 133:12802. https://doi.org/10.1115/1.4001073Huang W, Moon S, Ohsawa K (2016) Near-nozzle dynamics of diesel spray under varied needle lifts and its prediction using analytical model. Fuel 180:292–300. https://doi.org/10.1016/j.fuel.2016.04.042Sun Z-Y, Li G-X, Chen C et al (2015) Numerical investigation on effects of nozzle’s geometric parameters on the flow and the cavitation characteristics within injector’s nozzle for a high-pressure common-rail DI diesel engine. Energy Convers Manag 89:843–861. https://doi.org/10.1016/j.enconman.2014.10.047Devassy BM, Habchi C, Daniel E (2015) Atomization modelling of liquid jets using a two-surface density approach. At Sprays 25:47–80Moon S, Gao Y, Park S et al (2015) Effect of the number and position of nozzle holes on in- and near-nozzle dynamic characteristics of diesel injection. Fuel 150:112–122. https://doi.org/10.1016/j.fuel.2015.01.097Payri R, Salvador FJ, Carreres M, De la Morena J (2016) Fuel temperature influence on the performance of a last generation common-rail diesel ballistic injector. Part II: 1D model development, validation and analysis. Energy Convers Manag 114:376–391. https://doi.org/10.1016/j.enconman.2016.02.043Plamondon E, Seers P (2014) Development of a simplified dynamic model for a piezoelectric injector using multiple injection strategies with biodiesel/diesel-fuel blends. Appl Energy 131:411–424. https://doi.org/10.1016/j.apenergy.2014.06.039Postrioti L, Malaguti S, Bosi M et al (2014) Experimental and numerical characterization of a direct solenoid actuation injector for diesel engine applications. Fuel 118:316–328. https://doi.org/10.1016/j.fuel.2013.11.001Desantes JM, Salvador FJ, Lopez JJ, De la Morena J (2011) Study of mass and momentum transfer in diesel sprays based on X-ray mass distribution measurements and on a theoretical derivation. Exp Fluids 50:233–246. https://doi.org/10.1007/s00348-010-0919-8De la Morena J, Neroorkar K, Plazas AH et al (2013) Numerical analysis of the influence of diesel nozzle design on internal flow characteristics for 2-valve diesel engine application. At Sprays 23:97–118. https://doi.org/10.1615/AtomizSpr.2013006361Duke DJ, Schmidt DP, Neroorkar K et al (2013) High-resolution large eddy simulations of cavitating gasoline-ethanol blends. Int J Engine Res 14:578–589. https://doi.org/10.1177/1468087413501824Mitroglou N, McLorn M, Gavaises M et al (2014) Instantaneous and ensemble average cavitation structures in diesel micro-channel flow orifices. Fuel 116:736–742. https://doi.org/10.1016/j.fuel.2013.08.060Wang X, Li K, Su W (2012) Experimental and numerical investigations on internal flow characteristics of diesel nozzle under real fuel injection conditions. Exp Therm Fluid Sci 42:204–211. https://doi.org/10.1016/j.expthermflusci.2012.04.022Sou A, Pratama RH (2016) Effects of asymmetric inflow on cavitation in fuel injector and discharged liquid jet. At Sprays 26:939–959. https://doi.org/10.1615/AtomizSpr.2015013501Xue Q, Battistoni M, Powell CF et al (2015) An Eulerian CFD model and X-ray radiography for coupled nozzle flow and spray in internal combustion engines. Int J Multiph Flow 70:77–88. https://doi.org/10.1016/j.ijmultiphaseflow.2014.11.012Castilla R, Gamez-Montero PJ, Ertrk N et al (2010) Numerical simulation of turbulent flow in the suction chamber of a gearpump using deforming mesh and mesh replacement. Int J Mech Sci 52:1334–1342. https://doi.org/10.1016/j.ijmecsci.2010.06.009Parlak Z, Engin T (2012) Time-dependent CFD and quasi-static analysis of magnetorheological fluid dampers with experimental validation. Int J Mech Sci 64:22–31. https://doi.org/10.1016/j.ijmecsci.2012.08.006Chiatti G, Chiavola O, Palmieri F (2009) Spray modeling for diesel engine performance analysis. SAE Tech Pap 2009-01-0835. https://doi.org/10.4271/2009-01-0835Marcer R, Audiffren C, Viel A, et al (2010) Coupling 1D system AMESim and 3D CFD EOLE models for diesel injection simulation Renault. In: ILASS—Eur. 2010, 23rd Annu. Conf. Liq. At. Spray Syst., pp 1–10Desantes JM, Salvador FJ, Carreres M, Martínez-López J (2014) Large-eddy simulation analysis of the influence of the needle lift on the cavitation in diesel injector nozzles. Proc Inst Mech Eng D 229:407–423. https://doi.org/10.1177/0954407014542627Battistoni M, Xue Q, Som S (2016) Large-eddy simulation (LES) of spray transients: start and end of injection phenomena. Oil Gas Sci Technol 71:24. https://doi.org/10.2516/ogst/2015024CONVERGE is a trade mark of convergent science. https://convergecfd.comMacian V, Bermúdez V, Payri R, Gimeno J (2003) New technique for determination of internal geometry of a diesel nozzle with the use of silicone methodology. Exp Tech 27:39–43. https://doi.org/10.1111/j.1747-1567.2003.tb00107.xDabiri S, Sirignano WA, Joseph DD (2007) Cavitation in an orifice flow. Phys Fluids 19:72112. https://doi.org/10.1063/1.2750655Mohan B, Yang W, Chou SK (2014) Cavitation in injector nozzle holes—a parametric study. Eng Appl Comput Fluid Mech 8:70–81Salvador FJ, Hoyas S, Novella R, Martinez-Lopez J (2011) Numerical simulation and extended validation of two-phase compressible flow in diesel injector nozzles. Proc Inst Mech Eng D 225:545–563. https://doi.org/10.1177/09544070JAUTO1569Som S, Longman DE, Ramirez AI, Aggarwal S (2012) Influence of nozzle orifice geometry and fuel properties on flow and cavitation characteristics of a diesel injector. In: Fuel Inject. Automot. Eng., pp 112–126Desantes JM, Salvador FJ, Carreres M, Jaramillo D (2015) Experimental characterization of the thermodynamic properties of diesel fuels over a wide range of pressures and temperatures. SAE Int J Fuels Lubr 8:2015-01-0951. https://doi.org/10.4271/2015-01-0951Bosch W (1966) The fuel rate indicator: a new measuring instrument for display of the characteristics of individual injection. SAE Pap. 660749Payri R, Salvador FJ, Gimeno J, Bracho G (2008) A new methodology for correcting the signal cumulative phenomenon on injection rate measurements. Exp Tech 32:46–49. https://doi.org/10.1111/j.1747-1567.2007.00188.xPayri F, Payri R, Salvador FJ, Martínez-López J (2011) A contribution to the understanding of cavitation effects in diesel injector nozzles through a combined experimental and computational investigation. Comput Fluids 58:88–101. https://doi.org/10.1016/j.compfluid.2012.01.005Lichtarowicz AK, Duggins RK, Markland E (1965) Discharge coefficients for incompressible non-cavitating flow through long orifices. J Mech Eng Sci 7:210–219. https://doi.org/10.1243/JMES_JOUR_1965_007_029_02Lopez JJ, Salvador FJ, De la Garza OA, Arrègle J (2012) Characterization of the pressure losses in a common rail diesel injector. Proc Inst Mech Eng D 226:1697–1706. https://doi.org/10.1177/0954407012447020Salvador FJ, Carreres M, Jaramillo D, Martínez-López J (2015) Comparison of microsac and VCO diesel injector nozzles in terms of internal nozzle flow characteristics. Energy Convers Manag 103:284–299. https://doi.org/10.1016/j.enconman.2015.05.062LMS (2010) Imagine.Lab AMESim v.10. User’s manualPayri R, Salvador FJ, Martí-Aldaraví P, Martínez-López J (2012) Using one-dimensional modeling to analyze the influence of the use of biodiesels on the dynamic behavior of solenoid-operated injectors in common rail systems: detailed injection system model. Energy Convers Manag 54:90–99. https://doi.org/10.1016/j.enconman.2011.10.00

Blood Banking in Living Droplets

Blood banking has a broad public health impact influencing millions of lives daily. It could potentially benefit from emerging biopreservation technologies. However, although vitrification has shown advantages over traditional cryopreservation techniques, it has not been incorporated into transfusion medicine mainly due to throughput challenges. Here, we present a scalable method that can vitrify red blood cells in microdroplets. This approach enables the vitrification of large volumes of blood in a short amount of time, and makes it a viable and scalable biotechnology tool for blood cryopreservation.National Institutes of Health (U.S.) (NIH R21 EB007707)Wallace H. Coulter FoundationUnited States. Army Medical Research and Materiel Command (Acquisition Activity Cooperative Agreement RO1 A1081534)Center for Integration of Medicine and Innovative TechnologyUnited States. Army Medical Research and Materiel Command (Acquisition Activity Cooperative Agreement R21 AI087107)United States. Army. Telemedicine & Advanced Technology Research Cente

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