活塞连杆机构的外文和翻译综述Word文档格式.docx
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Abstract
Thispaperdealswithmodelingandsimulationofthedynamicsoftwocommonlyusedmechanisms,
(1)theCrankshaft–Connectingrod–Piston–Cylindersystem,and
(2)theUniversalJointsystem,usingtheBondGraphApproach.Thisalternativemethodofformulationofsystemdynamics,usingBondGraphs,offersarichsetoffeaturesthatinclude,pictorialrepresentationofthedynamicsoftranslationandrotationforeachlinkofthemechanismintheinertialframe,representationandhandlingofconstraintsatjoints,depictionofcausality,obtainingdynamicreactionforcesandmomentsatvariouslocationsinthemechanism,algorithmicderivationofsystemequationsinthefirstorderstate-spaceorcauseandeffectform,codingforsimulationdirectlyfromtheBondGraphwithoutderivingsystemequations,andsoon.
Keywords:
BondGraph,Modeling,Simulation,Mechanisms.
1Modeling
Dynamicsoftwocommonlyusedmechanisms,
(1)theCrankshaft–Connectingrod–Piston–Cylindersystem,and
(2)theUniversalJointsystem,aremodeledandsimulatedusingtheBondGraphApproach.Thisalternativemethodofformulationofsystemdynamics,usingBondGraphs,offersarichsetoffeatures[1,2].Theseinclude,pictorialrepresentationofthedynamicsoftranslationandrotationforeachlinkofthemechanismintheinertialframe,depictionofcauseandeffectrelationship,representationandhandlingofconstraintsatjoints,obtainingthedynamicreactionforcesandmomentsatvariouslocationsinthemechanism,derivationofsystemequationsinthefirstorderstate-spaceorcauseandeffectform,codingforsimulationdirectlyfromtheBondGraphwithoutderivingsystemequations.Usuallythelinksofmechanismsaremodeledasrigidbodies.
Inthiswork,wedevelopandapplyamultibondgraphmodelrepresentingbothtranslationandrotationofarigidbodyforeachlink.Thelinksarethencoupledatjointsbasedonthenatureofconstraint[3-5].Bothtranslationalandrotationalcouplingsforjointsaredevelopedandintegratedwiththedynamicsoftheconnectinglinks.Aproblemofdifferentialcausalityatlinkjointsariseswhilemodeling.Thisisrectifiedusingadditionalstiffnessanddampingelements.Itmakesthemodelmorerealistic,bringingineffectsofcomplianceanddissipationatjoints,withindefinabletolerancelimits.MultibondGraphmodelsfortheCrankshaft–Connectingrod–Piston–Cylindersystem,and,theUniversalJointsystem[6],aredevelopedusingtheBondGraphApproach.ReferenceframesarefixedoneachrigidlinkofthemechanismsusingtheDenavit-Hartenbergconvention[7].Thetranslationaleffectisconcentratedatthecenterofmassforeachrigidlink.Rotationaleffectisconsideredintheinertialframeitself,byconsideringtheinertiatensorforeachlinkaboutitsrespectivecenterofmass,andexpressedintheinertialframe.Themultibondgraphisthencausaledandcoding
inMATLAB,forsimulation,iscarriedoutdirectlyfromtheBondGraph.AsketchofthecrankshaftmechanismisshowninFig.1,anditsmultibondgraphmodelisshowninFig.2.AsketchoftheUniversaljointsystemisshowninFig.3,anditsmultibondgraphmodelisshowninFig.4.Resultsobtainedfromsimulationofthedynamicsofthesemechanismsarethenpresented.
1.1Crankshaft-ConnectingRod-Piston-CylinderMechanism
Fig.1showsthesketchofthe“Crankshaft–Connectingrod–Piston–Cylindersystem.”
Fig.1:
Crankshaft-ConnectingRod-Piston-CylinderMechanism.
Theindividualcomponentsareconsideredasrigidlinks,connectedatjoints.Thefirstmovinglinkisthecrank,thesecondlinkistheconnectingrodandthethirdlinkisthepiston.Aframeisfixedoneachlink.Thusframe1isfixedonlink1,frame2onlink2,andframe3onlink3.Afixedinertialframe0,whoseorigincoincideswithframe1,ischosen.However,itwillneitherrotatenortranslate.C1,C2andC3arecentresofmassofrespectivelinks.TheframesarefixedonrespectivelinksusingtheDenavit-Hartenbergconvention[4].
DynamicsofthesystemofFig.1ismodeledinthemultibondgraphshowninFig.2.Themodeldepictsrotationaswellastranslationforeachlinkinthesystem.Theleftsideofthebondgraphshowstherotationalpartandrightpartshowsthetranslationalpart.WerestrictanymotionbetweentheoriginofinertialframeOandpointonthelink1thatisO1byapplyingsourceofflowSfaszero.SimilarlywerestrictanyrelativemotionatpointA,distinguishedbyA1onlink1andA2onlink2,byapplyingsourceofflowSfaszero.Thepistonwhichislink3,isconstrainedtotranslateonlyalongtheX0direction.TranslationalongY0andZ0directionisconstrainedbyapplyingsourceofflowSfaszeroforthesecomponents.DifferentialcausalityiseliminatedbymakingtheK(1,1)elementofthestiffnessmatrix[K]betweenlink2andlink3aszero.
Additionalstiffnessanddampingelementsusedforeliminatingdifferentialcausalitymakethemodelmorerealistic,bringingineffectsofcomplianceanddissipationatjoints,withindefinabletolerancelimits.TheseviscoelasticelementsarerepresentedinthebondgraphbyusingCandRelements.
WehaveasourceofeffortSeatlink3,whichisthepressureforceactingonthepiston,althoughthisforceisalsoactingonlyinXdirection.
Fig.2:
MultibondgraphmodelfortheCrankshaft–Connectingrod–Piston–CylindersystemofFig.1.
1.2UniversalJointMechanism
TheFig.3showsthesketchofthe“UniversalJoint”mechanism.
Fig.3:
UniversalJointMechanism.
Ithasthreerigidlinks,twoareyokeswhichareattachedtorotatingshaftsandthemiddleoneisthecrossconnectingthetwoyokes.Theinertialframeisnumbered0,anditisfixed.Frame1isonlink1,frame2onthecrosswhichislink2,andframe3ontherightyokewhichislink3.Originoftheinertialframecoincideswiththatofframe1oflink1.Thelinks1and2areconnectedwitheachotherattwocoincidentendpointspointsA-A1onlink1andA2onlink2,andB-B1onlink1andB2onlink2.Similarlylinks2and3areconnectedattwopointsD-D2onlink2andD3onlink3,andE-E2onlink2andE3onlink3.
Link1rotatesaboutZaxiswithrespecttotheinertialframe.Theframe2islocatedatthecentreofmassofthelink2.Link2rotateswithrespecttothelink1indirectionZ2asshowninFig.3.Frame3alsocoincideswithframe2butitislocatedonthelink2.Theframe3onlink3rotateswithrespecttothelink2,aboutZ3,asshowninFig.3.ThebondgraphforthissystemisshowninFig.4.
Fig.4:
MultibondgraphfortheUniversalJointsystemofFig.
Theissueofdifferentialcausalityarisesforthismechanismalso.Itiseliminatedusingadditionalstiffnessanddampingelements.Asdiscussedearlier,thismakesthemodelmorerealistic,bringingineffectsofcomplianceanddissipationatjoints,withindefinabletolerancelimits.Therelativemotionbetweenthelinksatjoints,alongcertaindirections,isrestrainedbyapplyingthesourceofflowSfaszero.Theconstraintrelaxationistunedbychangingthevaluesofstiffnessanddampingatcorrespondingjoints.Herewerestrictthemotionofthelink3intwodirectionsYandZ,andallowmotioninXdirectionbyresolvingthesourceofflowinthreepartsandbyputtingSfaszeroinYandZdirectionsonly.Forthesimulation,anexcitationtorqueisappliedtolink1abouttheZdirection
2Simulation
TheresultsofcomputersimulationforthecrankshaftmechanismofFig.1arediscussedfirst.Theinitialpositionofthecrankshaftisat1θ=60owiththeX0axis.Itisthenreleasedundertheeffectofgravity.Theforceofgravityalsoactsontheconnectingrod.Noforceduetogaspressureisconsideredforthesimulationasitisnotthemainissueunderfocusforthispaper.TheupperrowinFig.5showsthedisplacementofthecentreofmassC1,asobservedandexpressedinFrame0.ItmovesinacirculararcabouttheZ0axis.ThefirstfigureinthelowerrowofFig.5showstheoscillationofthecrankshaft
abouttheZ0axisthroughchangeinorientationoftheunitvectorsofFrame1.ThesecondfigureinthesecondrowshowstheoscillationofthecentreofmassC1withtime.Thiscouldperhapsbeascribedtothenonlinearityimposedduetocouplingwiththeconnectingrod.
SimulationresultsfortheUniversaljointsystemarepresentedinFig.8.Aconstanttorqueisappliedtothedrivingshaftaboutitsaxis.Thedrivenshaftmakesanangleof5°
withtheaxisofthedrivingshaft.TheFirstrowshowstheresponseofthedrivingshaftwhichisthefirstlink.Thecomponentofangularmomentumofthedrivingshaftaboutitsaxisincreaseslinearly,whichisasexpected.Thefirsttwofiguresofthesecondrowshowthechangeinorientationofthecross,whichislink2.Angularmotionaboutallthreeaxesisclearlyvisible.ThedrivenshaftfollowsthemotionofthedrivershaftasisclearfromthethirdrowinFig.8.
3Conclusions
TheBondGraphapproachisusedtomodeldynamicsoftwocommonlyusedmechanisms,
(1)theCrankshaft–Connectingrod–Piston–Cylindersystem,and
(2)theUniversalJointsystem.Pictorialrepresentationofthedynamicsoftranslationandrotationforeachlinkofthemechanismintheinertialframe,representationandhandlingofconstraintsatjoints,depictionofcauseandeffectrelationships,codingforsimulationdirectlyfromtheBondGraphwithoutderivingsystemequations,havebeenexplainedinthiswork.MATLABbasedsimulationshavebeenpresentedandinterpretedforbo