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5 Additional Applications of Newton’s Laws • Friction • Drag Forces • Motion Along a Curved Path • The Center of Mass • Hk: 31, 43, 53, 57, 67, 81, 91, 101.

5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

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Page 1: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

5 Additional Applications of Newton’s Laws

• Friction

• Drag Forces

• Motion Along a Curved Path

• The Center of Mass

• Hk: 31, 43, 53, 57, 67, 81, 91, 101.

Page 2: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Friction

• Surface Force opposing relative motion

• Component of Contact Force (other component is the Normal Force)

• Characterized by coefficients (mu)

• Static (varies 0 to max)

• Kinetic (~ constant)

• Rolling (~ one tenth of kinetic)

Page 3: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Surface Dependence of Friction

Page 4: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Normal Force Dependence of Friction

• Contact area ~ to Normal Force

• Frictional Force ~ Normal Force

• Summary:

• Two factors affect frictional force;

• Surface composition

• Normal Force

• /

Page 5: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

5

Equations for Friction

Nss Ff max,Friction Static

Nkk Ff Friction Kinetic

Nrr Ff Friction Rolling

Page 6: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

6

Example Friction• Ex. 10kg block. FN = weight = mg = 98N.

Static coef. = 0.50; Kinetic coef. = 0.30.

N

Nf s49

)98)(50.0(max,

N

Nfk29

)98)(30.0(

Page 7: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Block at rest. Draw a Force Diagram for the block.

Page 8: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Three boxes are pushed by force F with v > 0 along a horizontal surface with k = 0.291.

F=26N

3kg5kg

2kgfk

NF

F

w

xx aF )10()98)(291.0(26

0mgFF Ny NmgFN 98

ssmax //25.010

)98)(291.0(26

Page 9: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Derive the Angle of Repose relation:

Maximum angle block remains at rest:

0sinmax mgfF sp

0cos mgFF Nn

sinmax mgFf Nss

cosmgFN

tancos

sin

sincos

s

s mgmg

Page 10: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Atwood with Friction. m1=1kg m2=2kg. Kinetic friction = 0.5.

CWCW ammfgmF )( 212

ssmmm

fgmaCW //9.4

21

8.9)5.0(6.19

21

2

Page 11: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Drag Forces

speedhigh at 2n and speed lowat 1n

:speedVary with

n

d bvF

throughmovesit fluid of type theand

object theof shape on the depends

when speed lat termina is

object fallingA :Speed Terminal Ex.

/1

b

b

mgv

mgbvn

T

n

Page 12: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Motion Along a Curved Path

• Force required turn and to change speed

• Coordinates usually used are F/B (tangential) and L/R (radial)

• Sum forces tangential = mass x tangential acceleration

• Sum forces L/R (radial centripetal) = mass x centripetal acceleration

• /

Page 13: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

What is the fastest speed the car can go without sliding? Assume the car has m = 1200kg and s = 0.92.

r

vmmgfF ssc

2max

r

vgs

2

smgrv s /3.20)7.45)(8.9)(92.0(

Page 14: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

A block loops the loop. Which force diagram is correct for when it passed point D?

Page 15: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Center of Mass Definition

21

2211

mm

xmxmxcm

21

2211

mm

vmvmvcm

21

2211

mm

amamacm

Page 16: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Center of Mass Acceleration

221121 amamFF

21

221121, )(

mm

amammmF extnet

cmextnet MaF ,

Page 17: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Center of Mass when Net External Force is Zero

• Zero Net Force implies center of mass acceleration is also zero. So if CM originally at rest, it remains at rest. If CM moving, its velocity remains same.

• Example: two people standing on ice push off one another

• /

Page 18: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Ex. Center of Mass. A 100kg person walks 6 feet forward in a 50kg canoe. How far did he move relative to the shore?

21

2211

21

2211

mm

xmxm

mm

xmxm

ftxx 621

22112211 xmxmxmxm zero beboth and Let 21 xx

02211 xmxm

ftxx 621 0)6( 2221 xmxm

06)( 1221 mxmm

ftmm

mx 4

50100

)100(66

21

12

ftftftx 2641

8Ch05ISM#13 toCompare

Page 19: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Summary

• Friction depends on Surface Composition and Normal Force

• Drag Force vary with speed

• Force required to move along curved path even at constant speed

• Center of Mass stays same when only internal forces operate

Page 20: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Can you stop in time?

Buggy rolls.You slide.

xnk

Mmx

aMmF

F

)(1

Page 21: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

xnk aMmF )(1

Given m = 75kg, M = 20kg, D = 3.5m, vo =1.1m/s. What frictional coefficient is needed?

xavv xo 222

Insert values, determine ax.

2

22

/1728.0

)5.3(2)1.1(0

sma

a

x

x

xk aMmmg )(

mg

aMm xk

))((

02233.0

)75(

)1728.0)(2075(

k

k g

Page 22: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Diagramming Refresher:

Page 23: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Accelerating with F2WD.

Stopping with 4W Disc-Brakes

Page 24: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

A 3kg box at rest on level surface with s = 0.55. What is the largest F acting 60° below horizontal for which the box remains at rest?

xy

060cos max sx fFF

04.2960sin FFF Ny

NF

F60

w

fs

NsFF 60cos

4.2960sin FFN

)4.2960sin(60cos FF s

17.16)4763.05.0( F

NF 683 (60° is close to maximum angle)

Page 25: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

vpc

vpg

Relative vs. Absolute Velocity

Page 26: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Which force diagram applies to the object at Point B?

Page 27: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Which force diagram applies to the object at Point C?

Page 28: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Assume mass = 1.2kg and radius = 45cm.If speed at Point D is 3.6m/s, what is the size of the normal force acting at Point D?

r

vmmgFF Nc

2

45.0

6.32.1)8.9)(2.1(

2

NF

NFN 8.22

-cen

+cen

Page 29: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Q. Assume mass = 1.2kg and radius = 45cm.If speed at Point B is 5.1m/s, what is the size of the normal force acting at Point B?

r

vmmgFF Nc

2

45.0

1.52.1)8.9)(2.1(

2

NF

NFN 81

+cen

-cen

Page 30: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Net

Given: T = 50N, = 30°, r = 1mFind: mg and v.

NTTFc 255.030sin 030cos mgTFy

NTmg 3.4330cos5030cos

18.9

3.4325

22 v

r

vmN

smv /378.23.43

)8.9)(25(

Page 31: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

The speed is now 6.5m/s and r = 1.0m. Angle, tension, mass?

r

vmTFc

2

sin mrL

Lr

03.1sin/

sin

0cos mgTFy

r

vmT

2

sin mgT cos

9.76

8.9

)5.6(tan

22

gr

v

Net

3.42cos// gmT

For example, if m = 1.0kg,

then T = 42.3N.

Page 32: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Q. The speed of a mass on a string of length L is 6.5m/s. The radius r = 2.0m. Find angle, tension, mass, and L.

1.65

6.19

)5.6(tan

22

gr

v

Net

9.23cos// gmT

For example, if m = 1.0kg,

then T = 23.9N.

mrL

Lr

20.2sin/

sin

Page 33: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Practice Q: What is F such that 0.5kg block stays at rest if all surfaces are frictionless?

Page 34: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Banked Turn:

Page 35: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Banked Turn:

Page 36: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Modified Atwood Machine with friction.

gmgmfF kCW 2121 sin

21

211 sincos

mm

gmgmgm

mass

Fa kCWCW

Let m1 = 2kg, m2 = 3kg, = 30°, sliding friction coeff. 0.44

)43.2(3)3(22 TgTgmFCW

NT 1.223.74.29

Objects are in CW motion.

cosmgFf kNkk

ssmggg

aCW //43.232

330sin)2(30cos)2)(44.0(

Page 37: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Q. Recalculate last problem with m1 = 6kg m2 = 1kg. (All else remaining the same)

)0.6(1)1(22 TgTgmFCW

NgT 8.15)0.6()1(

ssmggg

aCW //0.616

130sin)6(30cos)6)(44.0(

Page 38: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Practice Q: Find the variable relationships.

Page 39: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 40: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Figures

Page 41: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 42: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 43: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 44: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 45: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 46: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 47: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 48: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
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Page 52: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 53: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 54: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101
Page 55: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Q. Assume the car has m = 1200kg and s = 0.92.

How large is the frictional force if v = 15m/s?

r

vmfF sc

2

r

vmf s

2

Nf s 59087.45

151200

2

Page 56: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

5-3Drag Forces

Page 57: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Drag Forces

• Can be approximated as,

• Fdrag = bvn

• where b and n are constants

Page 58: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Example: Air drag, n = 2.

If b = 25N/(m/s)2, at what speed would the object be resisted by 10N?

2bvFd smv /632.025/10 22510 v

At what speed would the same object be resisted by 30N?

22530 v smv /095.125/30

Page 59: 5 Additional Applications of Newton’s Laws Friction Drag Forces Motion Along a Curved Path The Center of Mass Hk: 31, 43, 53, 57, 67, 81, 91, 101

Drag force grows quickly with v:

Terminal Velocity:

Reached when drag force equals weight force