classical mechanics lecture 22 - sfu
TRANSCRIPT
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Classical Mechanics Lecture 22
Today’sConcept: SimpleHarmonicMo7on:Mo#onofaPendulum
MechanicsLecture8,Slide1
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Grading
Unit14and15Ac7vityGuideswillnotbegraded
Pleaseturnin:! Unit14WriIenHomeworkonMon,Dec5! TheMini-labbookonyourSHMorKarateProject,Dec12
ThelastFlipItPhysicslectureisabonus.! notonexam! useitifyoumissedanypointsearlier! AlsousetheextraTipler&Moscaques7onsonF.P.forbonusandprep
FinalExam7me:Tue.,Dec.12,3:30pm
Finalexamroom:2600
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Howdoweknowwhentousethesinformulaorcosformulafortheposi7onoftheoscilla7ngsystem?Aretheybothviable?alsocanyouseethisface--> ( ͡° ͜ʖ ͡°)?
thisiskindoffromthelastlecturebuthowdoyougettheequa7onofx=Asin(ωt+φ)fromawordproblem?(ie.Howdoyouknowwahtφis?andisitcosorsin?)
Who'sthegeniuswhodecidedomegashouldhavetwomeanings?DidtheyrunoutofGreekleIers?Whydon'ttheyflyoverthereandgetsomemore?Itwouldprobablyhelpboosttheireconomyatthispoint.
Iamfindingitdifficulttounderstandhowthemomentofiner7aandtheradiusarebothbeingusedintheequa7on.Isn'tthemomentofiner7adependentontheradius?
talkingaboutharmonicmo7ons,Letsalldance"GANGNOMstyle",itsaperfectprac7calexample!
Forthetorsionpendulum,whatdidthelowercasekappa(κ, κ)represent?Whatcausesthatconstant?Thanks.
Howdoyouknowwhentousewhatformula?Intheprelecturetheydidn'texplainclearlyifyoucanusethesameformulaforapendulumwithamassaIachedtotheendasforapendulumwithoutamassaIachedtoit.
Your Comments
MechanicsLecture8,Slide2
despacito
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“ThereisatheorywhichstatesthatifeveranybodydiscoversexactlywhattheUniverseisforandwhyitishere,it
willinstantlydisappearandbereplacedbysomethingevenmorebizarreandinexplicable.”
MechanicsLecture8,Slide3
“Thereisanothertheorywhichstatesthatthishasalreadyhappened.”
Text
DouglasAdams
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Drillaholethroughtheearthandjumpin–whathappens?
Justforfun–youdon’tneedtoknowthis.
Iwanttoknowwhytheanswertolifeis42!
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Youwilloscillatelikeamassonaspringwithaperiodof84minutes.Ittakes42minutestocomeouttheotherside!
Drillaholethroughtheearthandjumpin–whathappens?
k = mg/RE
MechanicsLecture8,Slide5
Iwanttoknowwhytheanswertolifeis42!
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Theholedoesn’tevenhavetogothroughthemiddle–yougetthesameansweranywayaslongasthereisnofric7on.
MechanicsLecture8,Slide6
Iwanttoknowwhytheanswertolifeis42!
Youwilloscillatelikeamassonaspringwithaperiodof84minutes.Ittakes42minutestocomeouttheotherside!
Drillaholethroughtheearthandjumpin–whathappens?
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Thisisalsothesameperiodofanobjectorbi7ngtheearthrightatgroundlevel.
MechanicsLecture8,Slide7Justforfun–youdon’tneedtoknowthis.
Iwanttoknowwhytheanswertolifeis42!
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Panic!
“IstheresuchathingasRota7onalHarmonicMo7on?TherebeIernotbe...”
Yesthereis.
Areyouready?
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I
wire
θ
τ
Torsion Pendulum
Q:Intheprelecturetheequa7onforrestoringtorqueisgivenasτ=-κθinclockwisedirec7on..soiftherestoringtorqueisincounterclockwisedirec7onsthenwouldτbeposi7ve?
MechanicsLecture8,Slide8
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Atorsionpendulumisusedasthe7mingelementinaclockasshown.Thespeedoftheclockisadjustedbychangingthedistanceoftwosmalldisksfromtherota7onaxisofthependulum.Ifweadjustthediskssothattheyareclosertotherota7onaxis,theclockruns:
A)FasterB)Slower
Small disks
CheckPoint
MechanicsLecture8,Slide9
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Ifweadjustthediskssothattheyareclosertotherota7onaxis,theclockruns
A)FasterB)Slower
B)T=2pi*sqrt(I/MgRcm).IfRcmdecreases,Twillincrease,makingtheclockrunslower.
A)Themomentofiner7adecreases,sotheangularfrequencyincreases,whichmakestheperiodshorterandthustheclockfaster.
MechanicsLecture8,Slide10
CheckPoint
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Pendulum
Forsmallθ
θ
XCM
RCM
Mg
θ
arc-length = RCM θ
XCM
RCM
MechanicsLecture8,Slide11
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CM
pivot
θ
RCM
The Simple Pendulum
Thegeneralcase
θL
Thesimplecase
MechanicsLecture8,Slide12
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Iftheclockisrunningtoofast,theweightneedstobemovedA)UpB)Down
Iftheclockisrunningtoofastthenwewanttoreduceit'speriod,T,andtodothatweneedtoincreaseomega,thefrequencyitmoveswithandtodothatweneedtheposi7onofthecenterofmasstobefurtherfromthepivot,whichisachievedbymovingtheweightdown.
MechanicsLecture8,Slide14
CheckPoint
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M
pivot
θRCM
The Stick Pendulum
CM
MechanicsLecture8,Slide15
Same period
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InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtothecenterofthesames7ck.Inwhichcaseistheperiodofthependulumthelongest?
A)Case1B)Case2C)Same
Case1 Case2
Cisnottherightanswer.
Letsworkthroughit
CheckPoint
m
m
m
MechanicsLecture8,Slide16
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T = 2⇡
s23 Lg
T = 2⇡
s12 Lg
InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtoastringoflengthL/2?
Inwhichcaseistheperiodofthependulumlongest?
A)Case1B)Case2C)Same
Case1 Case2
m
MechanicsLecture8,Slide17
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Nowsupposeyoumakeanewpendulumbyhangingthefirsttwofromthesamepivotandgluingthemtogether.
Whatistheperiodofthenewpendulum?
A)T1 B)T2C)Inbetween
m
Supposeyoustartwith2differentpendula,onehavingperiodT1andtheotherhavingperiodT2.
T1
T2
T1 > T2
MechanicsLecture8,Slide18
m
m
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InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtothecenterofthesames7ck.Inwhichcaseistheperiodofthependulumthelongest?
A)Case1B)Case2C)Same
Nowletsworkthroughitindetail
Case1 Case2
m
MechanicsLecture8,Slide19
m
m
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Case2m
m
mCase 1
Letscompareforeachcase.
MechanicsLecture8,Slide20
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(A)
(B)
(C)
Case2m
m
mCase 1
Letscompareforeachcase.
MechanicsLecture8,Slide21
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Inwhichcaseistheperiodlongest?
A)Case1
B)Case2
C)Theyarethesame
m
Case1
Sowecanworkout
Case2
m
m
MechanicsLecture8,Slide22
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Angle(degrees)
%differen
cebetweenθ and
sinθ
- Exact expression
The Small Angle Approximation
θ
arc-length = RCM θ
XCM
RCM
MechanicsLecture8,Slide23
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Apendulumismadebyhangingathinhoola-hoopofdiameterDonasmallnail.Whatistheangularfrequencyofoscilla7onofthehoopforsmalldisplacements?(ICM=mR2forahoop)
A)
B)
C)
D
pivot(nail)
Clicker Question
MechanicsLecture8,Slide24
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Theangularfrequencyofoscilla7onofthehoopforsmall
displacementswillbegivenby
R
XCM
Useparallelaxistheorem:I = ICM + mR2
m
= mR2 + mR2 = 2mR2
pivot(nail)
MechanicsLecture8,Slide25
So