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1、S.Widnall16.07DynamicsFall2009LecturenotesbasedonJ.PeraireVersion2.0LectureL3-Vectors,MatricesandCoordinateTransformationsByusingvectorsanddefiningappropriateoperationsbetweenthem,physicallawscanoftenbewritteninasimpleform.SincewewillmakingextensiveuseofvectorsinDynamics,wewillsummarize
2、someoftheirimportantproperties.VectorsForourpurposeswewillthinkofavectorasamathematicalrepresentationofaphysicalentitywhichhasbothmagnitudeanddirectionina3Dspace.Examplesofphysicalvectorsareforces,moments,andvelocities.Geometrically,avectorcanberepresentedasarrows.Thelengthofthearrowre
3、presentsitsmagnitude.Unlessindicatedotherwise,weshallassumethatparalleltranslationdoesnotchangeavector,andweshallcallthevectorssatisfyingthisproperty,freevectors.Thus,twovectorsareequalifandonlyiftheyareparallel,pointinthesamedirection,andhaveequallength.Vectorsareusuallytypedinboldfac
4、eandscalarquantitiesappearinlightfaceitalictype,e.g.thevectorquantityAhasmagnitude,ormodulus,A=
5、A
6、.Inhandwrittentext,vectorsareoftenexpressedusingthe−→arrow,orunderbarnotation,e.g.A,A.VectorAlgebraHere,weintroduceafewusefuloperationswhicharedefinedforfreevectors.MultiplicationbyascalarI
7、fwemultiplyavectorAbyascalarα,theresultisavectorB=αA,whichhasmagnitudeB=
8、α
9、A.ThevectorB,isparalleltoAandpointsinthesamedirectionifα>0.Forα<0,thevectorBisparalleltoAbutpointsintheoppositedirection(antiparallel).Ifwemultiplyanarbitraryvector,A,bytheinverseofitsmagnitude,(1/A),weobtainaun
10、itvectorwhichisparalleltoA.Thereexistseveralcommonnotationstodenoteaunitvector,e.g.Aˆ,eA,etc.Thus,wehavethatAˆ=A/A=A/
11、A
12、,andA=AAˆ,
13、Aˆ
14、=1.1VectoradditionVectoradditionhasaverysimplegeometricalinterpretation.ToaddvectorBtovectorA,wesimplyplacethetailofBattheheadofA.ThesumisavectorCfromth
15、etailofAtotheheadofB.Thus,wewriteC=A+B.ThesameresultisobtainediftherolesofAarereversedB.Thatis,C=A+B=B+A.Thiscommutativepropertyisillustratedbelowwiththeparallelogramconstruction.Sincetheresultofaddingtwovectorsisalsoavector,wecanconsiderthesumofmultiplevectors.Itcaneasilybeverifiedth