Theoretical Analysis of Noise of Piston Knocking Cylinder Wall in Automotive Engines.docx
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Theoretical Analysis of Noise of Piston Knocking Cylinder Wall in Automotive Engines.docx
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TheoreticalAnalysisofNoiseofPistonKnockingCylinderWallinAutomotiveEngines
TheoreticalAnalysisofNoiseofPistonKnockingCylinderWallinAutomotiveEngines
XIAOYun-kui(肖云魁),LIShi-yi(李世义),CAOYa-juan(曹亚娟),
YANGWan-cheng(杨万成),FENGHan-sheng(冯汉生)
(1.SchoolofMechatronicsEngineering,BeijingInstituteofTechnology,Beijing100081,China;
2.MilitaryTransportationInstituteofTianjin,Tianjin300161,China)
Abstract:
Basedontheloadingconditionsofengine,applyingdifferencemethodtosolvethehydrodynamiclu—bricationequationofpistonskirtmovement,theforceactingonpistonskirtandthemomentonwristpinwere
obtained.AcomputerprogramforsimulatingthepistonsecondordermotionwasconductedtocalculatethelateralmotionoftheupperpartandthebottompartofpistonskirtsoftheengineofautomotivemodelCA1091.Fromthesimulatedresult,themaximalimpactingphaseandthemaximalimpactingregionofthepistonwereobtained.Theresultcanbeusedfordesigningengine,diagnosingthenoiseofpistonknockingcylinderwallandexplainingmanypracticalfaultphenomenaintheory.
Keywords:
pistonknockingcylinderwall;secondordermotion;faultdiagnosis
CLCnumber:
TH165;TK428Documentcode:
AArticleID:
1004.0579(2005)03.0284—05
Thenoiseofpistonknockingcylinderwall(PKCW)isoneofthemostfamiliarfaultphenomenainautomotiveengines.Whenthepiston-to-cylinderclearanceisbigandtheengineisrunningattheidlespeedthemetalknockingnoisewithaclearrhythmcanbeheardfromtheengine.Whenthefaultcylinderisflameoutthemetalknockingnoiseweakensordisappears.ThemildnoiseofPKCWisallowedinnormalengines,buttheenginewithheavynoiseofPKCWmustberepairedimmediately.Otherwise,thepistonwouldbebrokentopieces.TherearemanywaystodiagnosethenoiseofPKCW.InthepastseveralyearsdiagnosingthefaultofPKCWdependedfullyonrepair-expert’sexperience.Nowadayspeoplecandiagnosethefaultbymeansofinstruments.
Commonly,therearetwowaystoworkoutthetransversemovingtrajectoryofpiston.OneistosolvethepredigestedReynoldsequationandtheotheristosolveReynoldsequationdirectly.Inthispaperwecalculatetheoilfilmthicknessbetweenpistonandcylinderwallbasedondifferentstructureparametersanddifferentoperationalconditionsofenginewiththesecondmethod.Thevaluableresultswereobtained.
1KineticsEquationsofPistonSystem
Ontheplanenormaltowristpinaxis,theforceandmomentactingonpistonwouldbringthetinytranslationsandtherotationswithintheconfinementofthecylinderclearance,whicharecalledthesecondordermotionsofthepistonsystem.Bothmotionscanbedefinedbytheeccentricdistanceetandeboreccentricityεtandεb.ItisshowninFig.1.
Ifthefrictionsofthewristpinbearing,pistonringgroovesandpistonringfacesareneglected,basedontheconditionsofboththeforceequilibriumofpistonskirtandthemomentequilibriumofwristpin,thefollowingequationscanbededuced:
=
(1)
(2)
(3)
whereFgisthepush-forcethattheburninggasincombustionchamberactsonpiston;Fcisthetransverseinertiaforceofpiston;Fpisthetransverseinertiaforcebetweenwristpinandthesmallerendofconnectingrod;F’cistheaxialinertiaforceofpiston;F’pistheaxialinertiaforcebetweenwristpinandthesmallerendofconnectingrod;Misthemomentonwristpinthatoilfilmactsonpistonskirt;Mcisthepistoninertiamomentonwristpin;Fistheforceofoilfilm;Cpisthedistanceonx—axisbetweenpiston’saxisandwristpin’saxis;Cgisthedistanceonz—axisbetweenpistoncentroidandwristpincenter;aisthedistancebetweenthetopofpistonskirtandwristpincenter;bisthedistancebetweenthetopofpistonskirtandpistoncentroid;Listhelengthofpistonskirt;mpisisthepistonquality;mpinisthequalityofbothwristpinandsmallerendofrod;Ipisisthepistoninertiamomentonwristpincenter;e’’bisthesidewiseaccelerationofthebottomofpistonskirt;e’’tisthesidewiseaccelerationofthetopofpistonskirt;Ψistheangleincludedbetweenconnectingrodandcylinderboreaxis.
HydrodynamicLubricationEquationofCylinderSleeveandPiston:
Whenapplyingtheincompressibleliquidlubricantequationtoexpressthelubricatingeffectbetweenpistonskirtandcylinderbore,itcanbeexpressedas
(4)
wherePisthepressureofoilfilm;histheoilfilmthickness;isthed
ynamicalviscidityoflubricatingisthepistonradius;Uistheslidingspeedofpiston’sreciprocatingmotion(gainedfromcrankshaftandconnectingrodmechanism);tisthetime.Becauseofet,eb< (5) wherecistheradialclearancebetweenpistonandcylinderwall;f(y)istheaxialshapefunctionofpistonskirt. Thefollowingdimensionlessparametersareintroduced: εtdenotestheeccentricityofthetopofpistonskirt;εbdenotestheeccentricityofthebottomofpistonskirt;ωistheanglespeedofcrankshaft,Eq.(4)canberewrittenas ; ; ; ; ; ; ; (6) Whereε’tandε’barethefirstderivativesofεtandεbwithrespecttotimet.WiththeboundaryconditionsEq.(7),thenumericalsolutionofPcanbeevaluatedbymeansofdifferencemethods.Thenthedimension1essoi1filmforceFandmomentMcanbeevaluatedbyintegralfortheareaofP>0.Theintegralfunctionsare Toagivenpistonmechanism,λ,R,ωandUarefixedvalues.InEqs.(6)一(9),F’andM’dependontherelationsofε’t,ε’b,εtandεb.Therefore, 2AnalysisofPistonSecond0rderMotionResults AccordingtotherealcylinderchamberpressureofthetypeoftheengineofautomotivemodelCA1091,thesecondordermotionofpistoniscomputedbythemethoddiscussedabove.Variouskindsofparametersareasfollows: ThelengthofpistonskirtL=0.0755m,thepistonradiusR=0.05029m,thelengthofconnectingrodLl: 0.217m,theradiusofcrankshaftRl=0.05715m,thequalityofpiston,Mpis=0.82kg,thequalityofwristpin,Mpin=0.23kg.thepiston-to-cylinderclearancec=0.08,0.12,0.16mmrespectively,thedistanceonx-axisbetweenpiston’saxisandwristpin’saxisCp=0.001,0.002mrespectively,dynamicalviscidityoflubricantμ=0.016Pa·s,0.00745Pa·srespectively,rotaryspeedofcrankshaft,n=500,800,1600,2000,2400r/minrespectively.Selectingpartofgraphs,somevaluableresultsarediscussedasfollows: ①Fig.2andFig.3showεt,εb,ε’’tandε’’bcurvesonnorma1clearance0.08mmand0.24mmatdifferentspeeds.Themaximumsofε’’tandε’’boccurnearthetopdeadcenterofthecompressioncyclewhile;ε’’tandε’’bareapproachingzeroinotherplaces.Inordertoexpressclearlyx-axis.340°-380°Crankanglesareonlytaken.Atthenormalclearancethemaxima1dimensionlesstransversedisplacement(DTD)ofpistonskirtis0.22.Atclearance0.24mm.themaxima1DTDreaches0.99andthemaxima1dimensionlesstransverseacceleration(DTA)is8timesasbigasthatofthenormalcondition.ThusthenoiseofPKCWwil1bemoreobvio ②Fig.2andFig.3alsoshowthattheDTDandDTAofpistonattherotaryspeedsbelow1200r/minaremuchbiggerthanthoseattherotaryspeedsabove1600r/min. Atlowerrotaryspeedsofengine,thesyntheticalactionoftheburninggaspressureandthereciprocatinginertiaforceaswellasthefrictionforcesmakespistonrapidlychangeitstransversemovingdirectionnearthetopdeadcenterofenginecompressivecycle.Withtherotaryspeedrising.thesyntheticalactionofvariousforcesmakespistontransversemovementweakenandresultsinthenoiseofPKCWdecreasingundertheconditionofabnormalmatchingclearance. Fromtheanalyses①and②,wecanknowthatthesensorshouldbeplacedontheupperpartofcylinderbody,i.e.nearthetopdeadcenterofengine,andtherotaryspeedshouldbebelowthemiddlerangespeedofengine,ifweuseinstrumentstocheckthenoiseofPKCW. ③Fig.4showsεt,εb,ε’’tandε’’bcurvesatdifferentspeedsformatchingclearance0.24mmwiththecylinderflameout.FromFig.2andFig.3itcanbeknownthatwhenthecylinderisflameouttheDTDandtheDTAofpistondecreaseaccordingly.Intherangeoflowerandmiddlespeeds,themaximalDTDofpistonisonly0.4,whichcannotproducetheobviousnoiseofPKCW.ItindicatesthatwhentheloadofenginerisesthenoiseofPKCWbecomesbigger.Whenthecylinderisflameout,thenoiseofPKCWweakens.IfsomeonediagnosesthenoiseofPKCWbyhisexperience,whenhemakesthefaultcylinderflameoutandthenoiseofPKCWweakens.heisab1etojudgethefaultcylinderimmediate1y. ④ThedynamicalviscidityoflubricantsignificantlyaffectsthenoiseofPKCW.TheDTDofpistonwiththelubricantdynamica1viscidityof0.016Pa·sismuchsmallerthanthatofpistonwiththelubricantdynamicalviscidityof0.00745Pa·s.Withinthepropermatchingclearanceofpiston—to-cylinder.Thebiggerthedynamicalviscidityoflubricantis,thethickerthethicknessofoilfi1mwillbe,andthereisgreaterpossibilitytoavoidPKCW.Sincethedynamicalviscidityoflubricantdecreasesastemperatureincreases,ifthetemperatureistoohigh,thedynamicalviscidityoflubricantdecreasestempestuous1vandtheoilfilmofacertainthicknessbetweenpistonandcylindercannotbeformed,PKCWoccurseasily. ⑤PKCWmainlytakesplaceatthebottomofpistonskirt.EventhoughtheDTDonthetopofpistonskirtchangesgreatly,astheoilfilminthatpartisthickenough,thepossibilityofPKCWdecreases.ThereforealmostallthePKCWtakeplaceatthebottomofpistonskirt. Themodernmotorcarenginehighestrotationalspeedmayreach4000~6000r/min,pistoneachsecondneedstowalkseveraldozenstravelingsc
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