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Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

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Page 1: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Classical Mechanics Lecture 7

Today’sConcepts:Work&Kine6cEnergy

MechanicsLecture7,Slide1

Page 2: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

KarateWillnotdoSession3ofUnit8.

ItisaKaratething.

WewillonlymarkSession2ofunit8.

Youcandoitasa“project”inUnit14insteadoftheassignedprojectonthependulum.

Page 3: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Which Job?Allthreejobspaythesameamountofmoney.Whichonewouldyouchooseforyourcrew?

A.Job1

B.Job2

C.Job3

SESSION ONE: PHYSICAL WORK AND POWER30 min

The Concept of Physical Work

Suppose you are president of the Load 'n' Go Co. A local

college has three jobs available and will allow you to

choose which one you want before offering the other two

jobs to rival companies. All three jobs pay the same

amount of money. Which one would you choose for your

crew?

Figure 10-1: A description of jobs to bid on

!Activity 10-1: Choosing Your Job

Examine the descriptions of the jobs shown in Figure 10-1.

Which one would you be most likely to choose? Least likely to

choose? Explain the reasons for your answer.

Workshop Physics: Unit 10 – Work and Energy Page 10-3

Authors: Priscilla Laws, Robert Boyle, and John Luetzelschwab

© 1990-94 Dept. of Physics and Astronomy, Dickinson College Supported by FIPSE (U.S.

Dept. of Ed.) and NSF. Modified for SFU by N. Alberding, 2005, 2008.

A B

B

C

Page 4: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Joke of the day

Don'tdrinkandDERIVE!

B

Page 5: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Stuff you asked about:WHATISGOINGONWITHALLTHEINTEGRALS??????HELP:(Ihatesprings,butweshouldtalkaboutthem.sta6cfric6onEverythingisfineexcepttheworkdonebyGravityfarfromearthTheslideshadalotofinforma6onthatwasconfusinganditflewby.I

didn'thave6metounderstandwhatwasgoingon.ThedotproductisocnfusingPredymucheverything.Thisprelecturesortofwentovermyhead.I'll

definitelyhavetowatchitagain.Theconceptofposi6veandnega6veworkisveryconfusing.please

explain

MechanicsLecture7,Slide2

Page 6: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1
Page 7: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Your comments and questions

Will we have to use integrals to calculate work? clarification on under what circumstances the dot product

should be used would be helpful.Are you going to test us on the dot product or is it just a concept

you want us to know?

Page 8: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

The Dot Product

MechanicsLecture7,Slide3

Page 9: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

~A =A

x

ı + A

y

| + A

z

k

~B =B

x

ı + B

y

| + B

z

k

ı · ı =1| · | =1

k · k =1

ı · | =0

| · k =0

k · | =0

Dot Product using Unit Vectors

etc.

Page 10: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

~A · ~B =(A

x

ı + A

y

| + A

z

k) · (Bx

ı + B

y

| + B

z

k)

=(Ax

B

x

ı · ı + A

x

B

y

ı · | + · · · + A

z

B

y

k · j + A

z

B

z

k · k)=(A

x

B

x

⇥ 1 + A

x

B

y

⇥ 0 + · · · + A

z

B

y

⇥ 0 + A

z

B

z

⇥ 1)~A · ~B =(A

x

B

x

+ A

y

B

y

+ A

z

B

z

)

Dot Product in Rectangular Coordinates

Page 11: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

~A · ~B =(A

x

B

x

+ A

y

B

y

+ A

z

B

z

)

=|~A||~B| cos ✓

✓ = arccos

0BBBB@~A · ~B|~A||~B|

1CCCCA

Finding the angle between vectorsIfweknowthexyzcomponentsoftwovectorswecanfindtheanglebetweenthem:

therefore

Page 12: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

|⇥A| =|⇥B| = 5

⇥A · ⇥B =3 · 4 + 4 · 3 = 24

� = arccos

0BBBB@⇥A · ⇥B|⇥A||⇥B|

1CCCCA

� = arccos

24

25

!= arccos 0.96

=0.28 rad = 16

~A = 3ı + 4 |~B = 4ı + 3 |

Example

Page 13: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Work-Kinetic Energy TheoremTheworkdonebythenetforceFasitactsonanobjectthatmovesbetweenposi6onsr1and r2 isequaltothechangeintheobject’skine6cenergy:

MechanicsLecture7,Slide4

W =

~r2Z

~r1

~F · d~l

Page 14: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

W =

~r2Z

~r1

~F · d~l = ~F · ~d0BBBBBBBBB@

~r2Z

~r1

d~l = ~d

1CCCCCCCCCA

Work-Kinetic Energy Theorem: 1-D Example

Iftheforceisconstantandthedirec6onsaren’tchangingthenthisisverysimpletoevaluate:

MechanicsLecture7,Slide5

Inthiscase sincecos(0)=1

ThisisprobablywhatyourememberfromHighSchool.(Thenota6onmaybeconfusingthough.)

F d

= Fd

car

Page 15: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Clicker Question

Alightercarandaheaviervan,eachini6allyatrest,arepushedwiththesameconstantforceF.Aierbothvehiclestraveladistanced,whichofthefollowingstatementsistrue?(Ignorefric6on)

MechanicsLecture7,Slide6

A)TheywillhavethesamevelocityB)Theywillhavethesamekine6cenergyC)Theywillhavethesamemomentum

F d

F d

car

van

Page 16: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

~r2Z

~r1

~F · d~l = �K

Aforcepushingoversomedistancewillchangethekine6cenergy.

MechanicsLecture7,Slide7

Concept–veryimportant

Deriva6on–notsoimportant

θ

Page 17: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Work done by gravity near the Earth’s surface

MechanicsLecture7,Slide8

mgpat

h

Page 18: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

mg

dl1dy1

dx1

mg

dl1

dl2

dlN

Work done by gravity near the Earth’s surface

MechanicsLecture7,Slide9

= m~g · d~l1 + m~g · d~l1 + · · · + m~g · d~lN2

Page 19: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

mg

dl1

dl2

dlN

Work done by gravity near the Earth’s surface

MechanicsLecture7,Slide10

Δy

= m~g · d~l1 + m~g · d~l1 + · · · + m~g · d~lN

Page 20: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Work-Kinetic Energy Theorem

Ifthereareseveralforcesac6ngthenWistheworkdonebythenet(total)force:

MechanicsLecture7,Slide12

Youcanjustadduptheworkdonebyeachforce

Page 21: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

H

FreeFallFric6onlessincline String

CheckPoint

Threeobjectshavingthesamemassbeginatthesameheight,andallmovedownthesamever6caldistanceH.Onefallsstraightdown,oneslidesdownafric6onlessinclinedplane,andoneswingsontheendofastring.

MechanicsLecture7,Slide13

Inwhichcasedoestheobjecthavethebiggestnetworkdoneonitbyallforcesduringitsmo6on?

A)FreeFall B)Incline C)String D)Allthesame

Page 22: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

vp

Clicker Question

Threeobjectshavingthesamemassbeginatthesameheight,andallmovedownthesamever6caldistanceH.Onefallsstraightdown,oneslidesdownafric6onlessinclinedplane,andoneswingsontheendofastring.Whatistherela6onshipbetweentheirspeedswhentheyreachthebodom?

H

FreeFallFric6onlessincline Pendulum

A)vf > vi > vp B)vf > vp > vi C)vf = vp = vi

MechanicsLecture7,Slide14

v f vi

Page 23: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

CheckPoint / Clicker Question

Onlygravitywilldowork:Wg = Δ K

H

FreeFallFric6onlessincline String

A) vf > vi > vp B) vf > vp > vi C) vf = vp = vi

Wg = mgH

Δ K = 1/2 mv22

MechanicsLecture7,Slide15

Page 24: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

CheckPoint

Acardrivesupahillwithconstantspeed.WhichstatementbestdescribesthetotalworkWTOTdoneonthecarbyallforcesasitmovesupthehill?

About50%gotthisright…

A)WTOT = 0

B)WTOT > 0

C)WTOT < 0

v

MechanicsLecture7,Slide16

Page 25: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

v

Clicker Question

Acardrivesupahillwithconstantspeed.Howdoesthekine6cenergyofthecarchangeasitmovesupthehill?

A)ItincreasesB)ItstaysthesameC)Itdecreases

MechanicsLecture7,Slide17

Page 26: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

v

CheckPoint

Acardrivesupahillwithconstantspeed.WhichstatementbestdescribesthetotalworkWTOTdoneonthecarbyallforcesasitmovesupthehill?

A) WTOT = 0

B) WTOT > 0

C) WTOT < 0

A)Thechangeinkine6cenergyiszerobecausethevelocityisconstant.Bythework-kine6cenergytheorem,weknowthatworkmustalsobezero.

B)Theforceoffric6onbetweenthecar'swheelsandtherampexertaforceuptherampoverapar6culardistance.W=Fd,sotheworkisposi6ve.C)gravityisdownwardandcarmovesupthehill.

MechanicsLecture7,Slide18

Page 27: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

CheckPoint

Aboxsitsonthehorizontalbedofamovingtruck.Sta6cfric6onbetweentheboxandthetruckkeepstheboxfromslidingaroundasthetruckdrives.

µS

a

Theworkdoneontheboxbythesta6cfric6onalforceasthetruckmovesadistanceDis:

A)Posi6veB)Nega6veC)Zero

About60%gotthisright…

MechanicsLecture7,Slide21

Page 28: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Physics211Lecture7,Slide22

From Before

Aboxsitsonthehorizontalbedofamovingtruck.Sta6cfric6onbetweentheboxandthetruckkeepstheboxfromslidingaroundasthetruckdrives.

Ifthetruckmoveswithconstantaccelera6ngtotheleiasshown,whichofthefollowingdiagramsbestdescribesthesta6cfric6onalforceac6ngonthebox:

µS

a

A B C

Page 29: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

CheckPoint

MechanicsLecture7,Slide23

Theworkdoneontheboxbythesta6cfric6onalforceasthetruckmovesadistanceDis:

A)Posi6veB)Nega6veC)Zero

D

A)becausethedirec6onofthesta6cfric6onalforceandthedirec6ontheboxtravelsareallsame.

B)Sincethefric6onforcealwayshasoppositedirec6onfromthemovementdirec6on,theworkdoneisnega6ve

C)Fric6onkeepstheboxfromsliding,thusD=0,andworkdoneis0.

µS

a

F

Page 30: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

MechanicsLecture7,Slide24

Work done by a Spring

Page 31: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

MechanicsLecture7,Slide25

Iamconfusedabouttheposi6veworkandnega6veworkandalsotheposi6veandnega6veforcesforthespringproblems.

Inthisexamplethespringdoes–veworksince F andΔxareinoppositedirec6on.Theaxesdon’tmader.

Usetheformulatogetthemagnitudeofthework

Useapicturetogetthesign(lookatdirec6ons)

Page 32: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Aboxadachedatresttoaspringatitsequilibriumlength.YounowpushtheboxwithyourhandsothatthespringiscompressedadistanceD,andyouholdtheboxatrestinthisnewloca6on.

Duringthismo6on,thespringdoes:

A)Posi6veWorkB)Nega6veWorkC)Zerowork

MechanicsLecture7,Slide26

Clicker Question

D

Page 33: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Aboxadachedatresttoaspringatitsequilibriumlength.YounowpushtheboxwithyourhandsothatthespringiscompressedadistanceD,andyouholdtheboxatrestinthisnewloca6on.

Duringthismo6on,yourhanddoes:

A)Posi6veWorkB)Nega6veWorkC)Zerowork

Clicker Question

MechanicsLecture7,Slide27

D

Page 34: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

Aboxadachedatresttoaspringatitsequilibriumlength.YounowpushtheboxwithyourhandsothatthespringiscompressedadistanceD,andyouholdtheboxatrestinthisnewloca6on.

Duringthismo6on,thetotalworkdoneontheboxis:

A)Posi6veB)Nega6veC)Zero

Clicker Question

MechanicsLecture7,Slide28

D

Page 35: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

= GMem

1r2� 1

r1

!

MechanicsLecture7,Slide29

W =

~r2Z

~r1

~F(~r) · d~r = �r2Z

r1

GMemr2 dr

Gravity

Page 36: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

W = GMem

1r2� 1

r1

!A)Case1B)Case2C)Theyarethesame

InCase1wesendanobjectfromthesurfaceoftheearthtoaheightabovetheearthsurfaceequaltooneearthradius.

InCase2westartthesameobjectaheightofoneearthradiusabovethesurfaceoftheearthandwesenditinfinitelyfaraway.

InwhichcaseisthemagnitudeoftheworkdonebytheEarth’sgravityontheobjectbiggest?

Clicker Question

Case1 Case 2

MechanicsLecture7,Slide30

Page 37: Classical Mechanics Lecture 7 - Simon Fraser University · 2017. 10. 23. · Classical Mechanics Lecture 7 Today’s Concepts: Work & Kine6c Energy Mechanics Lecture 7, Slide 1

W = GMem

12RE� 1

RE

!= �GMem

2RE

W = GMem

11 �

12RE

!= �GMem

2RE

Case1 Case2

Case1:

2RE

RE

Same!

Clicker Question Solution

MechanicsLecture7,Slide31

Case2: