simulation of a diesel engine with variable geometry turbocharger … · 2017-08-10 · thomas, et...
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NomeNclatureCR DI Common rail direct injectionVGT Variable geometry turbochargerECU Engine control unitEGR Exhaust gas recirculationBSFC BrakespecificfuelconsumptionBMEP BrakemeaneffectivepressureIMEP IndicatedmeaneffectivepressurePMEP PumpingmeaneffectivepressureBTE BrakethermalefficiencyAFR AirfuelratioIC Inter coolerHFM HotFilmMass-flowEPC Electro-pneumaticPressureConverter
1. INtroductIoN Diesel engineswill continue tobe theprime-moversof
futurebattle tanksowing to their fuel economy,high torqueandeaseofmaintenance.Commonraildirectinjection(CRDI)technologywithelectronicenginecontrolislikelytoovercomethe challenges imposed by extreme weather conditionsand other hazards like zero visibility dusty terrains andwill
replacepresentmechanicalfuelinjectionsystemsinthebattletank.Modellingofaturbochargerisofinteresttotheenginedesignerastheworkdevelopedbytheturbinecanbeusedtodrive a compressor coupled to it. This positively influenceschargeairdensityandenginepowertoweightratio.Variablegeometryturbocharger(VGT)additionallyhasacontrollableset of nozzles which through a ring is normally electro-pneumaticallyactuatedbytheenginecontrolunit(ECU).Thisadditionaldegreeoffreedomoffersefficientmatchingof theeffective turbine area for awide range of enginemass flowrates.Atthedesignpoint,nozzlelessturbineisgenerally7percentlessefficientthantheturbinewithnozzlebladeswhereasatoffdesignpointsitperformsbetterthanturbinewithnozzleblades1.UsingVGT,thislossinefficiencycanbereducedbymatching incidencegasflowangle at the turbine rotor entryto the optimum incidence angle thereby reducing incidence losswhichisamajorlossatoffdesignoperationasprovenbyexperimental studies in2.Hence,aCRDIenginewithelectroniccontrol and VGT offers the advantage of closely matchedengine-turbochargercoupledoperationatalloperatingpoints.But multivariable nature of this control problemmakes thesystem complex and makes control strategies and controller design complicated. In the conventional approach, a mapof boost pressure as a function of engine speed and throttle
Simulation of a diesel engine with Variable Geometry turbocharger and Parametric Study of Variable Vane Position on engine Performance
Anand Mammen Thomas#,*,JensenSamuelJ.@,PaulPramodM.@, A.Ramesh@,R.Murugesan!,andA.Kumarasamy!
#Research & Innovation Centre, Chennai - 600 113, India @Indian Institute of Technology Madras, Chennai - 600 036, India
!Combat Vehicles Research and Development Establishment, Chennai - 600 054, India *E-mail: [email protected]
abStract
Modellingofaturbochargerisofinteresttotheenginedesignerastheworkdevelopedbytheturbinecanbeusedtodriveacompressorcoupledtoit.Thispositivelyinfluenceschargeairdensityandenginepowertoweightratio.Variablegeometryturbocharger(VGT)additionallyhasacontrollablenozzleringwhichisnormallyelectro-pneumaticallyactuated.Thisadditionaldegreeoffreedomoffersefficientmatchingoftheeffectiveturbineareaforawiderangeofenginemassflowrates.Closingofthenozzlering(vanestangentialtorotor)resultinmoreturbineworkanddeliverhigherboostpressurebut it also increases thebackpressureon theengine inducedby reducedturbineeffectivearea.Thisadverselyaffectsthenetenginetorqueasthepumpingworkrequiredincreases.Hence,theoptimumvanepositionforagivenengineoperatingpointistobefoundthroughsimulationsorexperimentation.Athermodynamicsimulationmodelofa2.2l4cylinderdieselenginewasdevelopedforinvestigationofdifferentcontrolstrategies.Modelfeaturesmapbasedperformancepredictionof theVGT.Performanceof theenginewassimulated for steady state operation and validatedwith experimentation.The results of the parametric study ofVGT’svanepositionontheengineperformancearediscussed.
Keywords: Thermodynamicsimulation;Variablegeometryturbocharger,Dieselengine
DefenceScienceJournal,Vol.67,No.4,July2017,pp.375-381,DOI:10.14429/dsj.67.11451 2017,DESIDOC
Received:21February2017,Revised:11May2017Accepted:18May2017,Onlinepublished:03July2017
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position is generally used for the closed loop controlof boost pressure where VGT is electro pneumaticallyactuatedtoachievethereferenceboostpressure3.Thismapisusuallypopulatedbytestbedcalibration.
Thermodynamic simulation is a very useful tool toarriveataninitialenginedesignandtodefineanoperationalenvelope. Commercial simulation software BOOST byM/sAVl is used to simulate the engine performance inthiswork4.A thermodynamic simulationmodelof a2.2l 4 cylinder diesel enginewas developed for investigationofdifferent control strategies.Model featuresmapbasedperformance prediction of the VGT as in5-7. Mass flowrate and efficiency maps of different pressure ratiosand turbocharger speeds for 5 different vane positionsincluding fullyopenposition (Fig.1. (a))andminimumflowposition(Fig.1.(b))weregivenbytheturbochargersupplier.Inthisapproach,turbochargerphysicsisassumedtobequasi-static with wave-action ignored. The results of simulationsand explores simulation as an alternative to engine test bedcalibration for arriving at reference boost pressure or VGTposition maps discussed.
simulateaircleaner,chargecoolerandVGTrespectively.Intakemanifoldismodelledasplenum‘Pl1’withfourintakerunnersconnecting it to the intake ports and cylinder.Cylinders areC1,C2,C3andC4withnumberingstartingfromdamperend.Exhaustmanifoldintheenginefeaturerunnerswithdifferentlength and centrally joined.Restriction ‘R1’which is addedtothetailpipetosimulateanybackpressureissetwithflowcoefficientsas1sinceenginesetupintestbeddoesnotfeatureanyafter-treatmentdevicesoranyotherdeviceswhichcouldhavecreatedbackpressuretotheengine.Arestriction‘R2’isusedtocontrolEGRflowrateandissetto0asEGRlinewasdisconnectedduringtheexperimentation.
2.2 Friction PowerFigure3showsfrictionpowerobtainedfromexperimental
cylinder pressure data with regulated coolant temperaturewhichwasusedinthemodel.
Figure 3. Friction data.Table 1. Engine specifications
Specifications
Type CRDIwithVGT
Ratedpower [hp] 120
Rated speed [rpm] 4000
Maxtorque [Nm] 280@(2400-2800rpm)
Noofcylinders [-] 4
Cylinderconfig. [-] I4
Sweptvolume [l] 2.179
Powerdensity [hp/l] 55.07
Bore [mm] 85
Stroke [mm] 96
Figure 2. thermodynamic model in aVl booSt.
2. tHermodYNamIc model 2.1 booSt layout
A 1-D thermodynamic model of an engine withspecifications as in Table 1, was created in AVl BOOSTsimulation software with VGT, charge air cooler, air filterconnectedasshowninFig.2.Inthemodel,SB1andSB2areused to simulate boundary conditions. Cl1, CO1 and TC1
2.3 combustionFigure4showscombustiondatawhichwasprovidedas
normalisedheatreleaseratescalculatedfromexperimentalin-cylinderpressure-trace.
2.4 VGtPerformancemapsofcentrifugalcompressor(Fig.5)and
radial inflow turbine (Figs.6and7)wereused tomodel theVGT.
Post processing and correction of the performanceparameterswithrespect tothereferencetestconditionswerecarried out prior to use in model as in8. Performancemapsof the turbine feature characteristics of the turbine for five
Figure 1. VGt open (a) and closed (b) nozzle blade positions.
(a) (b)
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differentVGTpositions including fully open as inFig. 1(a)andfullyclosedpositionasinFig.1(b).TurbochargerInertiausedis20kg.mm2.
3. INStrumeNtatIoN aNd eXPerImeNtatIoNEngine under consideration was instrumented with
thermocouples for temperature measurement and piezo-resistive pressure sensors for pressure measurement as inFig. 8. Additional parameters acquired were combustionrelated parameters using piezo-electric pressure transducer,turbocharger rotational speed using an eddy current type sensor andVGTposition.AirmassflowratewasmeasuredusinganHFM sensor. Experimentation facility with the test enginefeaturingCRDIandVGTissetupasshowninFig.9.
4. ValIdatIoN oF tHe model4.1 Steady State Performance Parameters
Asteadystateengineoperatingpointwith1800rpm,222Nm brake torque was selected for validation of the model.Major performance parameters are compared in Table 2.Resultsindicatethatpredictionofperformancebysimulation
is well within 5 per cent of measured data fromexperimentation.
4.2 Pressure trace comparisonPressuretracecomparisonsalsocorrelatewellas
showninFig.10withsimulatedpeakfiringpressureandcrankangleatpeakfiringpressurevalueswithin5percentofmeasuredvalues.
4.3 turbine Inlet Pressure comparisonOnly reliable measurement available for
verifying intra-cycle pulsations is the pressure tracein the exhaust manifold. Measuring instantaneouspulsatingtemperatureandmassflowarenotfeasiblewith conventional instrumentation. Hence, pressuretrace in the exhaust manifold measured from thecooled piezo-resistive pressure transducer wascomparedwiththesimulatedvalues.Matchingthesevales,itisevidentthatsimulatedturbineinletpressurepulsations correlateswellwith themeasured values
Figure 4. combustion data as rate of heat release.
Figure 5. compressor map.
Figure 7. turbine mechanical efficiency characteristics for different VGt positions.
Figure 6. Turbine mass flow characteristics for different VGT positions.
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to study theeffectofVGTvanepositionswitha full sweepfromfullyopenpositiontofullyclosedposition.VGTp in the graphsindicatesVGTpositionand0correspndstofullyclosedposition and VGTp1indicatesfullyopenposition(inFigs.12-18).Otherinputsinthemodelwerekeptsame.
Figure12showsthatvanepositioncorrespondingto60percentopengivesaminimumbrakespecificfuelconsumption(BSFC)whileextremevanepositionsresultinanincreaseinfuelconsumptionofabout4-5percent.Twocontradictingphysicaleffects-i.e,closingofvanesproducinghigherrotationalspeed(Fig.13)oftheturbochargertherebyresultinginanincreaseof turbinework (Fig. 14), compressorwork (Fig. 15), boostpressure(Fig.16)and‘indicatedmeaneffectivepressureforthe high pressure phase of the thermodynamic cycle’ (Fig.17) and also, closing of vane reduces effective turbine flowarea (Fig. 18) resulting inhigherbackpressure (Fig. 19)on
Figure 11. turbine inlet pressure pulsations comparison.
Figure 10. turbine inlet pressure pulsations comparison.
Figure 8. Instrumentation layout.
Figure 9. experimentation setup.
table 2. Validation of performance parameters
Performance parameter experimentation Simulation error
Speed [rpm] 1800 1800 0.00
Torque[Nm] 221.7 221.7 0.01
Power[kw] 41.8 41.8 0.02
BMEp [bar] 12.8 12.8 0.01
BSFC[g/kwhr] 224.0 232.5 -3.81
BTE [per cent] 38.3 36.3 5.25
AFR [-] 17.61 17.56 0.30
Airmassflowrate[g/s] 45.91 47.73 -3.96
Fuelflowrate[g/s] 2.6 2.7 -3.85
Fuelling[mg/stroke] 43.3 45.0 -3.85
Boost pressure [bar] 1.50 1.44 4.00
Turbo speed [rpm] 101473 98235 3.19
Air in [°C] 35 35 0.00
IC in [°C] 88.2 92.5 -4.89
IC out [°C] 64.2 66.0 -2.85
Turbine in [°C] 683.0 685.7 -0.40
Turbine out [°C] 606.0 640.1 -5.63
asshowninFig.11.HencemodelcanbereliablyappliedtogenerateboundaryconditionsforVGTturbinemodellingandtransientstudies.
5. aPPlIcatIoN oF tHe model: ParametrIc StudY oF VGt VaNe PoSItIoNValidationofthemodelwascarriedoutwithabaseVGT
position of 60 per cent open. Simulations were carried out
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theengineresultinginhigherpumpingmeaneffectivepressure(Fig. 20) during the gas exchange phase of thermodynamiccycle–explaintheBSFCvariationfromoptimum.
Also,turbineisnetropicefficiency(Fig.21)reduceseithersideoftheoptimumvaluebutthiseffectisnotstrongenoughtoreducetheturbinework(Fig.14)intheregiontotheleftofoptimumpoint,asthisisoffsetbyhigherrotationalspeedoftheturbocharger.
Figure 12. effect on bSFc.
Figure 13. effect on rotational speed of VGt.
Figure 14. effect on turbine work.
Figure 15. effect on compressor work
Figure 16 effect on boost Pressure.
Figure 17. effect on ImeP-HP.
Figure 18. Effect on effective flow area.
Figure 19. effect on engine back pressure.
Figure 20. effect on ImeP –Ge.
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6. coNcluSIoNSA thermodynamic model was developed for a 2.2 l
4 cylinder engine which was validated with steady stateexperimentation. Simulation results correlate well within 5percentofmeasuredvaluesofperformanceparametersfromexperimentation.ModelwasfurtherappliedtostudytheeffectofvariablevanepositionofVGTonengineperformance.AnoptimumpositionofVGTvaneisevidentfromtheresultswithreference to fuelconsumption.Studiesshows thatclosingofthevanes(nozzlering)resultinmoreturbineworkanddeliverhigher boost pressure but it also increases the back pressure ontheengineinducedbyreducedturbineeffectivearea.Thisadversely affects the net engine torque as pumping workrequiredincreases.Hence,thereisaneedtofindanoptimumboost pressuremap for the closed loop control of theVGTusingECUandEPC.Thus this studypresents simulationasan alternative to engine test bed calibration for arriving atreferenceboostpressureorVGTpositionmaps.
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7. lujan, J.M.; Galindo, J. & Serrano, J.R. Efficiencycharacterization of centripetal turbines under pulsatingflowconditions.SAEpaper2001-01-0272.
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acKNowledGmeNtS Authors wish to thank Dr V. Ramanujachari, Founder
Director, RIC, Dr V. Natarajan, Director, RIC and Dr P.Sivakumar,DSandDirector,CVRDEforgivingpermissiontopublishthework.
coNtrIbutorS
mr anand mammen thomas,completedBachelor’sinMechanicalEngineeringfromCollegeofEngineering,Trivandrum,in2007and currently pursuing Master’s in Mechanical Engineering at IIT Madras. Presently working as Scientist ‘C’ in Research& Innovation Centre, IIT Madras Research Park, Chennaiand is working on control strategies for a common rail directinjection armoured fightingvehicle engine.Hehasworkedondesigning anddeveloping engine subsystems like air filtrationand turbochargers. His research interests include : Modellingand control of transient response of turbo-charging systems.Contribution in the current study, he has carried out thethermodynamic simulations in the study and supported the experimentation and did some of the instrumentation of theengine.
mr Jensen Samuel J., completed his Masters in InternalCombustionEngineeringfromCollegeofEngineeringGuindy,AnnaUniversityChennai in2011.PresentlypursuinghisPhDfrom Indian Institute of Technology Madras and working onmodelling combustion for RT model-based control of Dieselengines during steady and transient operating conditions.Research interests include: ICengine testing,dataacquisition,physics-based modelling and control.Contribution in the current study, he has carried out theinstrumentation and experimentation of the engine in thestudy. mr Paul Pramod m.,completedhisBachelor’sinMechanicalEngineeringatIndianInstituteofTechnology,Madras.Currentlypursuing his Master’s in Automotive Engineering at RwTHAachen University, Germany and also working as studentworker in FEV Europe GmbH.Contribution in the current study, he has developed ECUapplication software for the engine. dr a. ramesh,obtainedhisPhD(Internalcombustionengines)from IITMadras and post doctoral research work from EcoleDesMinesDeNantes,France.HeisanInstituteChairProfessorof Mechanical Engineering and also head of the Center forContinuing Education in IITMadras. He has published over135 research papers on GDI and HCCI engines, alternativefuels and engine management. He has filed/obtained severalpatents.Contribution in thecurrentstudy,hehasarrivedat thecontrollogic of the CR DI engine and guided the overall work.
Figure 21. Effect on turbine efficiency.
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mr r. murugesan, is a post graduate engineer and workingas Scientist ‘F’ in Combat Vehicles R&D Establishment,Chennai.Hehasmorethan28yearsofexperienceandworkedextensivelyindesignanddevelopmentofdieselengineanditssub-systems forarmoured fightingvehicles and its evaluation.He is currently leading the Centre for Engineering AnalysisDivision (CEAD) in CVRDE.Contribution in the current study, he has supported overallwork and contributed to generation of the input data for thesimulations.
mr a. Kumarasamy, completedMasters from IITM,Chennaiin 1995. working as Scientist ‘G’ in CVRDE, Chennai andheading engine division. Developed compact cooling systemfor combat vehicles. Guided and upgraded power output ofanexistingengineandevaluatedat field conditions.Presentlyguiding a team for developing engines for 400 – 1500 hprange.Hisresearchinterestsincludedieselengineforarmouredfighting vehicles (AFVs) for 400 to 1500 hp range, compactcooling system for AFVs, efficient air filtration system forAFVs, advanced & efficient technologies for sub systems ofdiesel engine and its peripheral systems.Hehas initiated this study, reviewed theworkandcontributedto the integration of the cooling system of the engine understudy.