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Chapter4
PlanarMotionofaRigidBody§
4.1Basicconceptanddecompositionofrigidbodyplanarmotion
Maincontents§4.2
Velocityofanypointinaplanarmotion§4.3
Accelerationofanypointinaplanarmotion1.Whatisplanarmotionofarigidbody?Thedistancebetweenanypointinarigidbodyandafixedplanealwayskeepsunchangedduringitsmotion.Thismotionofrigidbodyiscalled
planarmotionofarigidbody.4.1Basicconceptanddecompositionofrigidbodyplanarmotion2.SimplificationofaplanarmotionTheplanarmotionofarigidbodycanbesimplifiedtoamotionofaplanegraphintheplaneitselfwithoutconsideringitsthickness.
(a)Connectingrodmotion(b)Simplificationofconnectingrodmotion4.1Basicconceptanddecompositionofrigidbodyplanarmotion3.EquationsofplanarmotionSTodeterminethemotionofaplanegraph,choosethefixedreferencesystemOxy,anarbitrarypointO'intheplanegraphS,anarbitrarylinesegmentO'M.Todeterminetheplanarmotionofarigidbody,onlythepositionofthelinesegmentO'Minthisgraphisneededtobedetermined.EquationsofplanarmotionAplanemotioncanberegardedasthecompositionofa
translation
androtation.4.1Basicconceptanddecompositionofrigidbodyplanarmotion4.Planarmotioncanbedecomposedintotranslationandrotation
Aplanemotionofarigidbodycanbedecomposedintoa
translationwithabasicpointanda
rotation
aboutanaxisthatpassesthroughthebasicpoint.Thevelocityandaccelerationofthe
translation
withabasicpoint
intheplanegraphdependson
theselectionof
thebasicpoint,however,theangularvelocityandaccelerationoftherotationabouttheselectedbasicpoint
doesn’tdependon
thechoiceofthebasicpoint.4.1BasicconceptanddecompositionofrigidbodyplanarmotionAThevelocityofpointAintheplanegraphSis,andtherotationalvelocityoftheplanegraphis.SelectAasthebasicpoint;ThemovingreferencesystemattachedtopointA;Thetransportmotionistranslationwiththebasicpoint
A;Therelativemotionisrotationaboutthebasicpoint
A.(1)Basicpointmethod
·BDeterminethevelocityofpointBintheplanegraph.4.2VelocityofanypointinaplanarmotionABTheorem:Forplanarmotionofarigidbody,thevelocityofanypointinthegraphcanbeobtainedasthevectorsumofthevelocityofthebasicpointandtherelativerotationalvelocitywithrespecttothebasicpoint.4.2Velocityofanypointinaplanarmotion
isverticaltothelinkofABallthetime,sotheprojectionofonABisvanish.Thevelocityprojectiontheorem:thevelocityprojectionsofanytwopointinaplanegraphonthelinelinkingthesetwopointsareidentical.(2)VelocityprojectiontheoremAB4.2Velocityofanypointinaplanarmotiona.Background
Ifapointwhosevelocityiszeroisselectedasthebasicpoint,theprocessoffindingthevelocityofanypointwillbegreatlysimplified.Therefore,itisnaturaltoaskifsuchapointexistsinanyinstant.Ifitdoesexist,howtofindsuchapoint?b.InstantaneouscenterofvelocityAtanyinstant,itmustexistasolepointwhosevelocityiszerointheplanegraphoritsexpandingarea,whichiscalledtheinstantaneousvelocitycenterofthisplanegraphatthisinstant.Foraplanegraph,itsinstantaneousvelocitycenteralwaysexistsuniquely.
(3)Instantaneouscenterofvelocitymethod4.2Velocityofanypointinaplanarmotionc.InstantaneouscenterofvelocitymethodConsideraplanegraph.TheinstantaneousvelocitycenterisP,andtheangularvelocityoftheplanegraphis.SelectinstantaneousvelocitycenterPisabasicpoint,thevelocityofanarbitrarypointAintheplanegraph:4.2Velocityofanypointinaplanarmotiond.MethodstodeterminetheinstantaneousvelocitycenterPA(1)Whenthevelocityofapointandtheangularvelocity
oftheplanegraphareknown,theinstantaneousvelocitycenter(pointP)canbedetermined,
pointPisinthedirectionofthelineformedbyrotatingthethrough90ºinthedirectionof
aroundpointA.4.2Velocityofanypointinaplanarmotion(2)Whenaplanegraphrollsalongafixedsurfacewithoutslipping,thecontactpointPbetweenthegraphandthefixedsurfacewillbetheinstantaneousvelocitycenter.
(3)WhenthedirectionsofthevelocitiesattwopointsAandBinagraphareknown,andisnotparallelto,drawlinesfromAandBperpendiculartorespectively,andthecrosspointPofthesetwolineswillbetheinstantaneousvelocitycenter.ABP4.2Velocityofanypointinaplanarmotion(4)WhenthevelocitiesoftwopointsAandBaregivenatanyinstant,and.Therearethreecases:ABP
Whenandpointtothesamedirection,but.DrawtheextensionlineofAB,thelinkinglineoftheendingsofand,thecrosspointofthesetwolineswillbetheinstantaneousvelocitycenter.Therotationdirectionofcanbedetermined,anditsmagnitudeis:◆ω
◆Whenandhaveoppositedirections,drawthelinkinglineoftheendingsofand,andthelineconnectingAB.Thecrosspointofthesetwolineswillbetheinstantaneousvelocitycenter.Therotationdirectionofcanbedetermined,anditsmagnitudeis:
ω4.2VelocityofanypointinaplanarmotionBPAB(5)ThevelocitiesoftwopointsAandBpointtothesamedirectionatanyinstant,,,buttheyarenotperpendiculartolineAB.Inthiscase,theinstantaneousvelocitycenterisindefinitelyfaraway,andtheangularvelocity
=0,i.e.allpointinthefigurehavethesamevelocityatthisinstantoftime.Suchamotioniscalledinstantaneoustranslation,buttheiraccelerationsarenotequal.
When,
theinstantaneousvelocitycenterisindefinitelyfaraway.Theplanegraphhasinstantaneoustranslation,=0,allpointsinthegraphhavethesamevelocityatthisinstantoftime,buttheiraccelerationsarenotequal.◆ω4.2VelocityofanypointinaplanarmotionAABAAttheinstant,theangularvelocityofthegraphis,angularaccelerationis,accelerationofapointAis
.DeterminetheaccelerationofanarbitrarypointBinthegraph.·
4.3
AccelerationofanypointinaplanarmotionBA1.
:
4.3
AccelerationofanypointinaplanarmotionBAB(1)thetangentialacceleration
(2)thenormalacceleration2.
:hastwocomponents:
4.3
AccelerationofanypointinaplanarmotionTheabsoluteaccelerationofpointB:Theorem:
Theaccelerationofanarbitrarypointisequaltothevectorsumofaccelerationofthebasicpoint,thetangentialandnormalaccelerationsoftheplanegraphrotatingaboutthebasicpoint.
4.3
Accelerationofanypointinaplanarmotionω1ⅠⅡO1OABCAnexternaltoothingplanetgearmechanismshowninthefigure.ThelinkingbarO1O=l,rotatesaboutaxisO1withauniformangularvelocityω1.ThebiggergearIIisfixed,theplanetgearIofradiusrrollsalongthegearIIwithoutsliding.AandBaretwopointsontheedgegearI,showninthefigure.FindtheaccelerationsofpointsAandB.Example
4-1
4.3
AccelerationofanypointinaplanarmotionBω1ⅠⅡO1ACωOSolution:GearIhasplanarmotion,thevelocityandaccelerationofitscentreO:TheinstantaneousvelocitycenterofgearⅠisC,
itsangularvelocity:1.Solvetheaccelerati
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