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ID:1514508
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时间:2017-11-12
《合力所做的功等于分力所做功的代数和》由会员上传分享,免费在线阅读,更多相关内容在教育资源-天天文库。
1、Chapter4WorkandEnergyWork:Everydaymeaning:anyactivitythatrequiresmuscularormentaleffort.Inphysics:theworkdoneonanobjectbyaforceinavectordisplacementistheirinnerproduct(scalar)—thesamemagnitudeofforce:positive,mines,zeroworkFrWork:varyingforcesoralon
2、gacurve合力所做的功等于分力所做功的代数和。TmgFExample:FindtheworkdonebyFwhenparticlemisslowlyliftedtothepresentposition.Solution1:Solution2:TmgF(1)平面直角坐标系(planarorthogonalcoordinatesystem)xyOxr0r1yFrs0s1FsWorkindifferentcoordinatesystems(2)平面“自然”坐标系(planarintrins
3、icsystem)r1rOr0F(,)(3)极坐标系(planarpolarsystem)Power(功率)Everydaymeaning:energyorforceInphysics:thetimerateatwhichworkisdone力的功率等于力与受力点速度的标积Summaryonwork功的性质(1)Generallyspeaking,workisdependentonthepath.功是过程量,一般与路径有关。(2)Workisascalarwithmagnitudea
4、ndsigns.功是标量,但有正负。(3)Workdonebyresultantofallforcesequals合力的功为各分力的功的代数和。Casestudy1:Workdonebygravitation引力的功两个质点之间在万有引力作用下相对运动时,以M所在处为原点,M指向m的方向为矢径r的正方向。m受的引力方向与矢径方向相反。m在M的万有引力的作用下从a点运动到b点,万有引力的功:Gravitationalwork:independentofthepathofthebody;depend
5、sonlyonthestartingandendingpoints引力的功:与路径无关,仅仅取决于起始和终点的位置Casestudy2:WorkdonebyelasticforceskOabkOacbOakkOabkOa<0Workdonebyelasticforces:弹力的功independentofthepathofthebody;dependsonlyonthestartingandendingpointsRuleofsigns:正负号W<0,外力做功,W>0,弹力做功“Work”can
6、bestoredandrecovered.“功”可以储存和释放Conservativeandnonconservativeforces:保守力和非保守力Workdonebyaconservativeforce保守力的功:(1)Reversible,“work”canbestoredina“BANK”;可逆,功可以被储存(2)Independentofthepathofthebody;与路径无关(3)Zeroworkforclosedpath.闭合路径做功为零ABL1L2等价Energyisdef
7、inedastheabilitytodowork.Workisdefinedasthetransferofenergy.Thewaterissaidtopossesskineticenergysinceitismoving.Itgetsthisenergybecauseitisfallingthroughagravitationalfield.Potentialenergy(势能)Energyassociatedwiththepositionofasystem.Storedinasystem,
8、laterrecovered.与相互作用物体的位置有关的能量。Workbyconservativeforcespotentialenergy势能的增量等于保守力所做功的负值.(1)保守力做功势能GravitationalpotentialenergyElasticpotentialenergy(2)势能保守力梯度:Example:findgravityfromgravitationalpotentialV=mgySolution:(3)1DEnergydiagram一维势能曲线xU(x)
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