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Classical Mechanics Lecture 22 Today’s Concept: Simple Harmonic Mo7on: Mo#on of a Pendulum Mechanics Lecture 8, Slide 1

Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

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Page 1: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Classical Mechanics Lecture 22

Today’sConcept: SimpleHarmonicMo7on:Mo#onofaPendulum

MechanicsLecture8,Slide1

Page 2: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Grading

Unit14and15Ac7vityGuideswillnotbegraded

Pleaseturnin:! Unit14WriIenHomeworkonMon,Dec5! TheMini-labbookonyourSHMorKarateProject,Dec12

ThelastFlipItPhysicslectureisabonus.! notonexam! useitifyoumissedanypointsearlier! AlsousetheextraTipler&Moscaques7onsonF.P.forbonusandprep

FinalExam7me:Tue.,Dec.12,3:30pm

Finalexamroom:2600

Page 3: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

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

Page 4: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

“ThereisatheorywhichstatesthatifeveranybodydiscoversexactlywhattheUniverseisforandwhyitishere,it

willinstantlydisappearandbereplacedbysomethingevenmorebizarreandinexplicable.”

MechanicsLecture8,Slide3

“Thereisanothertheorywhichstatesthatthishasalreadyhappened.”

Text

DouglasAdams

Page 5: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Drillaholethroughtheearthandjumpin–whathappens?

Justforfun–youdon’tneedtoknowthis.

Iwanttoknowwhytheanswertolifeis42!

Page 6: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Youwilloscillatelikeamassonaspringwithaperiodof84minutes.Ittakes42minutestocomeouttheotherside!

Drillaholethroughtheearthandjumpin–whathappens?

k = mg/RE

MechanicsLecture8,Slide5

Iwanttoknowwhytheanswertolifeis42!

Page 7: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Theholedoesn’tevenhavetogothroughthemiddle–yougetthesameansweranywayaslongasthereisnofric7on.

MechanicsLecture8,Slide6

Iwanttoknowwhytheanswertolifeis42!

Youwilloscillatelikeamassonaspringwithaperiodof84minutes.Ittakes42minutestocomeouttheotherside!

Drillaholethroughtheearthandjumpin–whathappens?

Page 8: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Thisisalsothesameperiodofanobjectorbi7ngtheearthrightatgroundlevel.

MechanicsLecture8,Slide7Justforfun–youdon’tneedtoknowthis.

Iwanttoknowwhytheanswertolifeis42!

Page 9: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Panic!

“IstheresuchathingasRota7onalHarmonicMo7on?TherebeIernotbe...”

Yesthereis.

Areyouready?

Page 10: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

I

wire

θ

τ

Torsion Pendulum

Q:Intheprelecturetheequa7onforrestoringtorqueisgivenasτ=-κθinclockwisedirec7on..soiftherestoringtorqueisincounterclockwisedirec7onsthenwouldτbeposi7ve?

MechanicsLecture8,Slide8

Page 11: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Atorsionpendulumisusedasthe7mingelementinaclockasshown.Thespeedoftheclockisadjustedbychangingthedistanceoftwosmalldisksfromtherota7onaxisofthependulum.Ifweadjustthediskssothattheyareclosertotherota7onaxis,theclockruns:

A)FasterB)Slower

Small disks

CheckPoint

MechanicsLecture8,Slide9

Page 12: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Ifweadjustthediskssothattheyareclosertotherota7onaxis,theclockruns

A)FasterB)Slower

B)T=2pi*sqrt(I/MgRcm).IfRcmdecreases,Twillincrease,makingtheclockrunslower.

A)Themomentofiner7adecreases,sotheangularfrequencyincreases,whichmakestheperiodshorterandthustheclockfaster.

MechanicsLecture8,Slide10

CheckPoint

Page 13: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Pendulum

Forsmallθ

θ

XCM

RCM

Mg

θ

arc-length = RCM θ

XCM

RCM

MechanicsLecture8,Slide11

Page 14: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

CM

pivot

θ

RCM

The Simple Pendulum

Thegeneralcase

θL

Thesimplecase

MechanicsLecture8,Slide12

Page 15: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Iftheclockisrunningtoofast,theweightneedstobemovedA)UpB)Down

Iftheclockisrunningtoofastthenwewanttoreduceit'speriod,T,andtodothatweneedtoincreaseomega,thefrequencyitmoveswithandtodothatweneedtheposi7onofthecenterofmasstobefurtherfromthepivot,whichisachievedbymovingtheweightdown.

MechanicsLecture8,Slide14

CheckPoint

Page 16: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

M

pivot

θRCM

The Stick Pendulum

CM

MechanicsLecture8,Slide15

Same period

Page 17: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtothecenterofthesames7ck.Inwhichcaseistheperiodofthependulumthelongest?

A)Case1B)Case2C)Same

Case1 Case2

Cisnottherightanswer.

Letsworkthroughit

CheckPoint

m

m

m

MechanicsLecture8,Slide16

Page 18: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

T = 2⇡

s23 Lg

T = 2⇡

s12 Lg

InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtoastringoflengthL/2?

Inwhichcaseistheperiodofthependulumlongest?

A)Case1B)Case2C)Same

Case1 Case2

m

MechanicsLecture8,Slide17

Page 19: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Nowsupposeyoumakeanewpendulumbyhangingthefirsttwofromthesamepivotandgluingthemtogether.

Whatistheperiodofthenewpendulum?

A)T1 B)T2C)Inbetween

m

Supposeyoustartwith2differentpendula,onehavingperiodT1andtheotherhavingperiodT2.

T1

T2

T1 > T2

MechanicsLecture8,Slide18

m

m

Page 20: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

InCase1as7ckofmassmandlengthLispivotedatoneendandusedasapendulum.InCase2apointpar7cleofmassmisaIachedtothecenterofthesames7ck.Inwhichcaseistheperiodofthependulumthelongest?

A)Case1B)Case2C)Same

Nowletsworkthroughitindetail

Case1 Case2

m

MechanicsLecture8,Slide19

m

m

Page 21: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Case2m

m

mCase 1

Letscompareforeachcase.

MechanicsLecture8,Slide20

Page 22: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

(A)

(B)

(C)

Case2m

m

mCase 1

Letscompareforeachcase.

MechanicsLecture8,Slide21

Page 23: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Inwhichcaseistheperiodlongest?

A)Case1

B)Case2

C)Theyarethesame

m

Case1

Sowecanworkout

Case2

m

m

MechanicsLecture8,Slide22

Page 24: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Angle(degrees)

%differen

cebetweenθ and

sinθ

- Exact expression

The Small Angle Approximation

θ

arc-length = RCM θ

XCM

RCM

MechanicsLecture8,Slide23

Page 25: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Apendulumismadebyhangingathinhoola-hoopofdiameterDonasmallnail.Whatistheangularfrequencyofoscilla7onofthehoopforsmalldisplacements?(ICM=mR2forahoop)

A)

B)

C)

D

pivot(nail)

Clicker Question

MechanicsLecture8,Slide24

Page 26: Classical Mechanics Lecture 22 - SFU.caa clock as shown. The speed of the clock is adjusted by changing the distance of two small disks from the rotaon axis of the pendulum. If we

Theangularfrequencyofoscilla7onofthehoopforsmall

displacementswillbegivenby

R

XCM

Useparallelaxistheorem:I = ICM + mR2

m

= mR2 + mR2 = 2mR2

pivot(nail)

MechanicsLecture8,Slide25

So