Download PHYS101

Document related concepts

Old quantum theory wikipedia , lookup

Inertia wikipedia , lookup

Quantum vacuum thruster wikipedia , lookup

Symmetry in quantum mechanics wikipedia , lookup

Tensor operator wikipedia , lookup

Equations of motion wikipedia , lookup

Laplace–Runge–Lenz vector wikipedia , lookup

Classical central-force problem wikipedia , lookup

Accretion disk wikipedia , lookup

Theoretical and experimental justification for the Schrödinger equation wikipedia , lookup

Photon polarization wikipedia , lookup

Relativistic mechanics wikipedia , lookup

Angular momentum wikipedia , lookup

Newton's laws of motion wikipedia , lookup

Angular momentum operator wikipedia , lookup

Momentum wikipedia , lookup

Relativistic angular momentum wikipedia , lookup

Transcript
IntroductoryPhysics
PHYS101
Dr RichardH.CyburtOfficeHours
TRF9:30-11:00am
AssistantProfessorofPhysics
F12:30-2:00pm
Myoffice:402cintheScienceBuilding
Myphone:(304)384-6006
Meetingsmayalsobearrangedatothertimes,
byappointment
Myemail:[email protected]
Inpersonoremailisthebestwaytogetahold
Checkmyscheduleonmyofficedoor.
ofme.
PHYS101
PHYS101:IntroductoryPhysics
400
Lecture:8:00-9:15am,TRScienceBuilding
Lab1:3:00-4:50pm,FScienceBuilding304
Lab2:1:30-3:20pm,MScienceBuilding304
Lab3:3:30-5:20pm,MScienceBuilding304
Lab20:6:00-7:50pm,MScienceBuilding304
PHYS101
MasteringPhysicsOnline
GotoHYPERLINK"http://www.masteringphysics.com."www.masteringphysics.com.
◦ UnderRegisterNow,selectStudent.
◦ Confirmyouhavetheinformationneeded,thenselectOK!Registernow.
RCYBURTPHYS101),andchooseContinue.
◦ Enteryourinstructor’sCourseID(
◦ EnteryourexistingPearsonaccountusername andpassword andselectSignin.
◦ YouhaveanaccountifyouhaveeverusedaPearsonMyLab &Masteringproduct,suchasMyMathLab,MyITLab,MySpanishLab,or
MasteringChemistry.
◦ Ifyoudon’thaveanaccount,select Create andcompletetherequiredfields.
◦ Selectanaccessoption.
◦ Entertheaccesscodethatcamewithyourtextbookorwaspurchasedseparatelyfromthebookstore.
PHYS101
Midterm2
Therewillbeabonusassignment,basedonyourexam
◦
◦
◦
◦
Willearnyouextrapointsonyourexam
Itwillbeonlineasahomework
Youmustdobetteronthisassignment,thanyourtesttogetbonuspoints
Bonus=30%x(Homework– Midterm)
BonusHomeworkisOnline,dueOct17,12:59pm (justbeforelabsstartfortheday)
AfterBonusHWisdue,therewillbeasignoutsheetinmyoffice
◦ Youmustsigntogetyourexam
PHYS101
IntroductoryPhysics
PHYS101
DouglasAdams
Hitchhiker’sGuidetotheGalaxy
PHYS101
You’realreadyknowphysics!
Youjustdon’tnecessarilyknowtheterminologyand
languageweuse!!!
PhysicsofNASCAR
PhysicsofAngerBirds
PHYS101
Inclass!!
PHYS101
Thislecturewillhelpyouunderstand:
ConservationofMomentum
InelasticCollisions
Momentum&Collisionsin2D
AngularMomentum
PHYS101
Section9.4
Conservationof
Momentum
©2015PearsonEducation,Inc.
ConservationofMomentum
Theforcesactingontwoballs
duringacollisionforman
action/reactionpair.They
haveequalmagnitudebut
oppositedirections(Newton’s
thirdlaw).
Ifthemomentumofball1
increases,themomentumof
ball2willdecreasebythe
sameamount.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Thereisnochangeinthetotal
momentumofthesystem no
matterhowcomplicatedthe
forcesarebetweentheparticles.
Thetotalmomentumofthe
systemisconserved.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Internalforces actonly
betweenparticleswithina
system.
Thetotalmomentumofa
systemsubjectedtoonly
internalforcesisconserved.
©2015PearsonEducation,Inc.
QuickCheck9.7
Youawakeinthenighttofindthatyourlivingroomisonfire.Yourone
chancetosaveyourselfistothrowsomethingthatwillhitthebackof
yourbedroomdoorandcloseit,givingyouafewsecondstoescapeout
thewindow.YouhappentohavebothastickyballofclayandasuperbouncySuperballnexttoyourbed,boththesamesizeandsamemass.
You’veonlytimetothrowone.Whichwillitbe?Yourlifedependson
makingtherightchoice!
◦ ThrowtheSuperball.
◦ Throwtheballofclay.
◦ Itdoesn’tmatter.Throweither.
©2015PearsonEducation,Inc.
QuickCheck9.7
Youawakeinthenighttofindthatyourlivingroomisonfire.
Youronechancetosaveyourselfistothrowsomethingthatwill
hitthebackofyourbedroomdoorandcloseit,givingyouafew
secondstoescapeoutthewindow.Youhappentohavebotha
stickyballofclayandasuper-bouncySuperball nexttoyourbed,
boththesamesizeandsamemass.You’veonlytimetothrow
one.Whichwillitbe?Yourlifedependsonmakingtheright
choice!
◦ ThrowtheSuperball.
Larger Dp Þ more impulse to door
◦ Throwtheballofclay.
◦ Itdoesn’tmatter.Throweither.
©2015PearsonEducation,Inc.
QuickCheck9.8
Amosquitoandatruckhaveahead-oncollision.Splat!Whichhasalarger
changeofmomentum?
◦
◦
◦
◦
Themosquito
Thetruck
Theyhavethesamechangeofmomentum.
Can’tsaywithoutknowingtheirinitialvelocities.
©2015PearsonEducation,Inc.
QuickCheck9.8
Amosquitoandatruckhaveahead-oncollision.Splat!Whichhasalarger
changeofmomentum?
◦
◦
◦
◦
Themosquito
Thetruck
Theyhavethesamechangeofmomentum.
Can’tsaywithoutknowingtheirinitialvelocities.
Momentum is conserved, so Dpmosquito + Dptruck = 0.
Equal magnitude (but opposite sign) changes in momentum.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Externalforcesareforcesfromagents
outsidethesystem.
Externalforcescan changethemomentum
ofthesystem.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Thechangeinthetotalmomentumis
isthenetforceduetoexternalforces.
Ifthetotal momentumofthesystemdoesnotchange.
Anisolatedsystem isasystemwithnonetexternalforceactingonit,leaving
themomentumunchanged.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Thelawofconservationofmomentumforanisolatedsystemiswritten
Thetotalmomentumafteraninteractionisequaltothetotal
momentumbeforetheinteraction.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Sincemomentumisavector,wecanrewritethelawofconservationof
momentumforanisolatedsystem:
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off
Twoiceskaters,SandraandDavid,
standfacingeachotheronfrictionlessice.
Sandrahasamassof45kg,Davidamass
of80kg.
Theythenpushofffromeachother.
Afterthepush,Sandramovesoff
ataspeedof2.2m/s.
WhatisDavid’sspeed?
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off(cont.)
PREPARE Thetwoskatersinteract
witheachother,buttheyforman
isolatedsystembecause,foreach
skater,theupwardnormalforceof
theicebalancestheirdownward
weightforcetomake
Thusthetotalmomentumofthesystemofthetwoskatersisconserved.
FIGURE9.17showsabefore-and-aftervisualoverviewforthetwoskaters.
Thetotalmomentumbeforetheypushoffis
becausebothskatersareatrest.Consequently,thetotalmomen-tumwill
stillbe0aftertheypushoff.
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off(cont.)
SOLVE Sincethemotionisonly
inthex-direction,we’llneedto
consideronlyx-componentsof
momentum.
WewriteSandra’sinitialmomentumas
(pSx)i =mS(vSx)i,
wheremS ishermassand(vSx)i herinitialvelocity.
Similarly,wewriteDavid’sinitialmomentumas(pDx)i =mD(vDx)i.
Boththesemomentaarezerobecausebothskatersareinitiallyatrest.
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off(cont.)
Wecannowapplythe
mathematicalstatementof
momentumconservation,
Equation9.15.Writingthe
finalmomentumofSandraas
mS(vSx)f andthatofDavid
asmD(vDx)f ,wehave
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off(cont.)
Solvingfor(vDx)f ,wefind
Davidmovesbackwardwithaspeed of1.2m/s.
©2015PearsonEducation,Inc.
Example9.5Speedoficeskaterspushing
off(cont.)
Noticethatwedidn’tneed
toknowanydetailsaboutthe
forcebetweenDavidand
SandrainordertofindDavid’s
finalspeed.Conservationof
momentummandates this
result.
ASSESS ItseemsreasonablethatSandra,whosemassislessthanDavid’s,would
havethegreaterfinalspeed.
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Text:p.265
©2015PearsonEducation,Inc.
LawofConservationofMomentum
Text:p.265
©2015PearsonEducation,Inc.
ItDependsontheSystem
Thegoalistochoose
asystemwhere
momentumwillbe
conserved.
Foraskateboarder,if
wechoosejustthe
person,thereisa
nonzeronetforceon
thesystem.
Ifwechoosethesystemtobethepersonand thecart,thenetforceiszeroand
themomentumisconserved.
©2015PearsonEducation,Inc.
ExampleProblem
Jackstandsatrestonaskateboard.
ThemassofJackandtheskateboardtogetheris75kg.
Ryanthrowsa3.0kgballhorizontallytotherightat4.0m/stoJack,whocatches
it.
WhatisthefinalspeedofJackandtheskateboard?
©2015PearsonEducation,Inc.
Explosions
Anexplosion iswhenthe
particlesofthesystem
moveapartafterabrief,
intenseinteraction.
Anexplosionistheopposite
ofacollision.
Theforcesareinternal
forcesandifthesystemis
isolated,thetotalmomentum
isconserved.
©2015PearsonEducation,Inc.
QuickCheck9.10
Thetwoboxesareonafrictionlesssurface.Theyhadbeensittingtogetherat
rest,butanexplosionbetweenthemhas
justpushedthemapart.Howfastisthe2-kgboxgoing?
◦
◦
◦
◦
◦
1m/s
2m/s
4m/s
8m/s
There’snotenoughinformationtotell.
©2015PearsonEducation,Inc.
QuickCheck9.10
Thetwoboxesareonafrictionlesssurface.Theyhadbeensittingtogetherat
rest,butanexplosionbetweenthemhas
justpushedthemapart.Howfastisthe2-kgboxgoing?
◦
◦
◦
◦
◦
1m/s
2m/s
4m/s
8m/s
There’snotenoughinformationtotell.
©2015PearsonEducation,Inc.
QuickCheck9.11
The1-kgboxisslidingalongafrictionlesssurface.Itcollideswithandsticksto
the2-kgbox.Afterward,thespeedofthetwoboxesis
◦
◦
◦
◦
◦
0m/s
1m/s
2m/s
3m/s
There’snotenoughinformationtotell.
©2015PearsonEducation,Inc.
QuickCheck9.11
The1-kgboxisslidingalongafrictionlesssurface.Itcollideswithandsticksto
the2-kgbox.Afterward,thespeedofthetwoboxesis
◦
◦
◦
◦
◦
0m/s
1m/s
2m/s
3m/s
There’snotenoughinformationtotell.
©2015PearsonEducation,Inc.
Example9.7Recoilspeedofarifle
A30gballisfiredfroma
1.2kgspring-loadedtoyrifle
withaspeedof15m/s.What
istherecoilspeedoftherifle?
PREPARE Astheballmoves
downthebarrel,thereare
complicatedforcesexerted
ontheballandontherifle.However,ifwetakethesystemtobetheball+ rifle,
theseareinternal forcesthatdonotchangethetotalmomentum.
©2015PearsonEducation,Inc.
Example9.7Recoilspeedofarifle(cont.)
Theexternal forcesofthe
rifle’sandball’sweightsare
balancedbytheexternalforce
exertedbythepersonholding
therifle,so
Thisis
anisolatedsystemandthe
lawofconservationof
momentumapplies.
FIGURE9.20showsavisualoverviewbeforeand
aftertheballisfired.We’llassumetheballisfiredinthe+x-direction.
©2015PearsonEducation,Inc.
Example9.7Recoilspeedofarifle(cont.)
SOLVE Thex-componentofthe
totalmomentumisPx = pBx + pRx.
Everythingisatrestbeforethetriggerispulled,
sotheinitialmomentumiszero.
Afterthetriggerispulled,theinternalforceof
thespringpushestheballdownthebarrelandpushestheriflebackward.
Conservationofmomentumgives
©2015PearsonEducation,Inc.
Example9.7Recoilspeedofarifle(cont.)
Solvingfortherifle’svelocity,wefind
Theminussignindicatesthat
therifle’srecoilistotheleft.
Therecoilspeed is0.38m/s.
©2015PearsonEducation,Inc.
Example9.7Recoilspeedofarifle(cont.)
ASSESS Realriflesfiretheir
bulletsatmuchhigher
velocities,andtheirrecoil
iscorrespondinglyhigher.
Shootersneedtobrace
themselvesagainstthe
“kick”oftherifleback
againsttheirshoulder.
©2015PearsonEducation,Inc.
Section9.5Inelastic
Collisions
©2015PearsonEducation,Inc.
InelasticCollisions
Aperfectlyinelastic
collision isacollisionin
whichthetwoobjectsstick
togetherandmovewitha
commonfinalvelocity.
Examplesofperfectly
inelasticcollisionsinclude
clayhittingthefloorand
abulletembeddingitself
inwood.
©2015PearsonEducation,Inc.
QuickCheck9.9
Thetwoboxesareslidingalongafrictionlesssurface.Theycollideandstick
together.Afterward,thevelocityofthe
twoboxesis
◦
◦
◦
◦
◦
2m/stotheleft
1m/stotheleft
0m/s,atrest
1m/stotheright
2m/stotheright
©2015PearsonEducation,Inc.
QuickCheck9.9
Thetwoboxesareslidingalongafrictionlesssurface.Theycollideandstick
together.Afterward,thevelocityofthe
twoboxesis
◦
◦
◦
◦
◦
2m/stotheleft
1m/stotheleft
0m/s,atrest
1m/stotheright
2m/stotheright
©2015PearsonEducation,Inc.
Example9.8Aperfectlyinelasticcollision
ofrailroadcars
[InsertFigure9.23]
Inassemblingatrainfrom
severalrailroadcars,two
ofthecars,withmasses
2.0´ 104 kgand4.0´ 104 kg,
arerolledtowardeachother.
Whentheymeet,theycoupleandsticktogether.
Thelightercarhasaninitialspeedof1.5m/s;thecollisioncausesittoreverse
directionat0.25m/s.
Whatwastheinitialspeedoftheheaviercar?
©2015PearsonEducation,Inc.
Example9.8Aperfectlyinelasticcollision
ofrailroadcars(cont.)
PREPARE Wemodelthecars
asparticlesanddefinethe
twocarsasthesystem.This
isanisolatedsystem,soits
totalmomentumisconserved
inthecollision.Thecarsstick
together,sothisisaperfectly
inelasticcollision.
FIGURE9.23showsavisualoverview.We’vechosentoletthe
2.0´ 104 kgcar(car1)startoutmovingtotheright,so(v1x)i isapositive1.5m/s.
Thecarsmovetotheleftafterthecollision,sotheircommonfinalvelocityis(vx)f
= −0.25m/s.Youcanseethatvelocity(v2x)i mustbenegativeinorderto“turn
around”bothcars.
©2015PearsonEducation,Inc.
Example9.8Aperfectlyinelasticcollision
ofrailroadcars(cont.)
SOLVE Thelawofconservationofmomentum,(Px)f = (Px)i,is
wherewemadeuseofthefactthatthecombinedmass
m1 + m2 movestogetherafterthecollision.
©2015PearsonEducation,Inc.
Example9.8Aperfectlyinelasticcollision
ofrailroadcars(cont.)
Wecaneasilysolveforthe
initialvelocityofthe
4.0´ 104 kgcar:
©2015PearsonEducation,Inc.
Example9.8Aperfectlyinelasticcollision
ofrailroadcars(cont.)
Thenegativesign,whichwe
anticipated,indicatesthat
theheaviercarstartedout
movingtotheleft.Theinitial
speedofthecar,whichwe
wereaskedtofind,is
1.1m/s.
ASSESS Thekeystepinsolvinginelasticcollisionproblemsisthatbothobjects
moveafterthecollisionwiththesamevelocity.Youshouldthuschooseasingle
symbol(here,(vx)f)forthiscommonvelocity.
©2015PearsonEducation,Inc.
ExampleProblem
A10gbulletisfiredintoa1.0kgwoodblock,whereitlodges.
Subsequentlytheblockslides4.0macrossafloor(μk =0.20forwoodonwood).
Whatwasthebullet’sspeed?
©2015PearsonEducation,Inc.
Section9.6Momentum
andCollisions
inTwoDimensions
©2015PearsonEducation,Inc.
MomentumandCollisioninTwo
Dimensions
Whenthemotionofthecollisionsoccurintwo
dimensions,wemustsolveforeachcomponent
ofthemomentum:
Inthesecollisions,the
individualmomentacan
changebutthetotal
momentumdoesnot.
©2015PearsonEducation,Inc.
ExampleProblem
Twopucksofequalmass100gcollideonanairhockeytable.
Neglectfriction.
Priortothecollision,puck1travelsinadirectionthatcanbeconsideredthe+xaxisat1m/s,andpuck2travelsinthe–y-directionat2m/spriortothecollision.
Afterthecollision,puck2travels30degreesabovethe+x-direction(between+x
and+y)at0.8m/s.
Whatisthevelocity(directionandspeed)ofpuck1afterthecollision?
Howdoesthefinalkineticenergycomparetotheinitialkineticenergy?
©2015PearsonEducation,Inc.
Section9.7Angular
Momentum
©2015PearsonEducation,Inc.
AngularMomentum
Momentumisnotconserved
foraspinningobjectbecause
thedirectionofmotionkeeps
changing.
Still,ifitweren’tforfriction,a
spinningbicyclewheelwould
keepturning.
Thequantitythatexpressesthis
ideaforcircularmotioniscalled
angularmomentum.
©2015PearsonEducation,Inc.
AngularMomentum
WecancalculatetheangularmomentumL.
Newton’ssecondlawgivestheangularacceleration:
Wealsoknowthattheangularaccelerationisdefinedas
Ifwesetthoseequationsequalandrearrange,wefind
©2015PearsonEducation,Inc.
AngularMomentum
Forlinearmotion,theimpulse-momentumtheoremiswritten
Thequantity Iωistherotationalequivalentoflinearmomentum,soitis
reasonabletodefineangularmomentumL as
TheSIunitsofangularmomentumarekg× m2/s.
©2015PearsonEducation,Inc.
AngularMomentum
©2015PearsonEducation,Inc.
ConservationofAngularMomentum
Angularmomentumcanbewritten
Ifthenetexternaltorqueonanobjectiszero,thenthechangeinangular
momentumiszeroaswell:
©2015PearsonEducation,Inc.
ConservationofAngularMomentum
Thetotalangularmomentum isthesumoftheangularmomenta ofallthe
objectsinthesystem.
Ifnonetexternaltorqueactsonthesystem,thenthelawofconservationof
angularmomentumiswritten
©2015PearsonEducation,Inc.
Example9.11Analyzingaspinningice
skater
Aniceskaterspinsaroundonthetipsofhisbladeswhileholdinga5.0kg
weightineachhand.Hebeginswithhisarmsstraightoutfromhisbody
andhishands140cmapart.Whilespinningat2.0rev/s,hepullsthe
weightsinandholdsthem50cmapartagainsthisshoulders.Ifweneglect
themassoftheskater,howfastishespinningafterpullingtheweightsin?
©2015PearsonEducation,Inc.
Example9.11Analyzingaspinningice
skater(cont.)
PREPARE Thereisnoexternaltorqueactingonthesystem
consistingoftheskaterandtheweights,sotheirangular
momentumisconserved.FIGURE9.29showsabefore-and-aftervisualoverview,
asseenfromabove.
©2015PearsonEducation,Inc.
Example9.11Analyzingaspinningice
skater(cont.)
SOLVE Thetwoweightshave
thesamemass,moveincircles
withthesameradius,andhave
thesameangularvelocity.Thus
thetotalangularmomentumis
twicethatofoneweight.Themathematicalstatementofangularmomentum
conservation,If wf =Iiwi,is
©2015PearsonEducation,Inc.
Example9.11Analyzingaspinningice
skater(cont.)
Becausetheangularvelocity
isrelatedtotherotation
frequencyf byw =2pf,this
equationsimplifiesto
Whenhepullstheweightsin,hisrotationfrequencyincreasesto
©2015PearsonEducation,Inc.
Example9.11Analyzingaspinningice
skater(cont.)
ASSESS Pullingintheweights
increasestheskater’sspinfrom
2rev/sto16rev/s.Thisis
somewhathighbecausewe
neglectedthemassoftheskater,
butitillustrateshowskatersdo“spinup”bypullingtheirmassintowardthe
rotationaxis.
©2015PearsonEducation,Inc.
ExampleProblem
Bicycleriderscanstayuprightbecauseatorqueisrequiredtochangethe
directionoftheangularmomentumofthespinningwheels.
Abikewithwheelswitharadiusof33cmandamassof1.5kg(each)travelsata
speedof10mph.
Whatistheangularmomentumofthebike?Treatthewheelsofthebikeas
thoughallthemassisattherim.
©2015PearsonEducation,Inc.