Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

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Chapter 6 •Circular Motion, Orbits, and Gravity

Transcript of Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Page 1: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Chapter 6

• Circular Motion, Orbits, and Gravity

Page 2: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Slide 6-23

Uniform Circular Motion

Page 3: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

For uniform circular motion, the acceleration

A. is parallel to the velocityB. is directed toward the center of

the circleC. is large for a larger orbital the

same speedD. is always due to gravity

is paral

lel to

the ve

locity

is dire

cted to

ward th

e cente

r...

is lar

ge for a

large

r orb

ital th

...

is alw

ays due to

gravit

y

0% 0%0%

100%

Page 4: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Forces in Circular Motion

Slide 6-24

22

2

net , toward center of circle

v = r

va = r

rmv

F = ma = r

Page 5: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Time of Circular Motion

𝑓 =1𝑇

The frequency is just the inverse of the period

Example of frequency units:revmin

𝑣=2𝜋𝑟𝑇

𝑣=2𝜋 𝑟𝑓

Page 6: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

What happens when speed decreases and radius decreases?

𝑎=𝑣2

𝑟

Page 7: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Comparing centripetal accelerations

Rank the acceleration of the following uniform circular motions from smallest to largest:

𝑎=𝑣2

𝑟

1 2 3 4 5

𝑣=2𝜋 𝑟𝑓

𝑎=(2𝜋𝑟𝑓 )2

𝑟=4𝜋  2𝑟 𝑓 2

They’re all going to have so we just need to find for each one

Page 8: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Comparing centripetal accelerations

Rank the acceleration of the following uniform circular motions from smallest to largest

1 2 3 4 5

𝑟1 𝑓 12

𝑎=𝑣2

𝑟𝑣=2𝜋 𝑟𝑓

(10cm )(50revmin )

2

𝑟2 𝑓 22

(20cm )(50revmin )

2

𝑟3 𝑓 32

(20cm )(100revmin )

2

𝑟 4 𝑓 42

( 40cm )(100revmin )

2

𝑟5 𝑓 52

( 40 cm )(200revmin )

2

Page 9: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Driving on a curvy road

𝑎=𝑣2

𝑟

𝑎=𝑣2

𝑟

𝑎=0

Page 10: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Problem solving uniform circular motion

𝑎=𝑣2

𝑟

𝑣=2𝜋 𝑟𝑓

Page 11: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A level curve on a country road has a radius of 150 m. What is the maximum speed at which this curve can be safely negotiated on a rainy day when the coefficient of friction between the tires on a car and the road is 0.40?

Slide 6-28

Problem solving uniform circular motion

Page 12: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A level curve on a country road has a radius of 150 m. What is the maximum speed at which this curve can be safely negotiated on a rainy day when the coefficient of friction between the tires on a car and the road is 0.40?

Slide 6-28

𝑓 𝑠=𝜇𝑠𝑁

𝑓 𝑠=𝜇𝑠𝑚𝑐𝑔¿𝑚𝑐𝑣2

𝑟 𝑣=√𝜇𝑠𝑔𝑟

Problem solving uniform circular motion

Page 13: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

When a car turns a corner on a level road, which force provides the necessary centripetal

acceleration?

A. FrictionB. TensionC. Normal ForceD. Air resistanceE. Gravity

Fricti

on

Tensio

n

Normal F

orce

Air res

istance

Gravity

76%

2%10%

0%

12%

Page 14: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A coin sits on a rotating turntable.

1. At the time shown in the figure, which arrow gives the direction of the coin’s velocity?

Additional Questions

Slide 6-45

Page 15: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

AnswerA coin sits on a rotating turntable.

1. At the time shown in the figure, which arrow gives the direction of the coin’s velocity?

A

Slide 6-46

Page 16: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A coin sits on a rotating turntable.

2. At the time shown in the figure, which arrow gives the direction of the frictional force on the coin?

Additional Questions

Slide 6-47

Page 17: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

AnswerA coin sits on a rotating turntable.

2. At the time shown in the figure, which arrow gives the direction of the frictional force on the coin? D

Slide 6-48

Page 18: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A coin sits on a rotating turntable.

3. At the instant shown, suppose the frictional force disappeared. In what direction would the coin move?

Additional Questions

Slide 6-49

Page 19: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Answer

A

A coin sits on a rotating turntable.

3. At the instant shown, suppose the frictional force disappeared. In what direction would the coin move?

Slide 6-50

Page 20: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A ball moves CW in circular motion. What happens when it reaches the opening?

A. AB. BC. CD. D

A B C D

0%0%

95%

5%

Page 21: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A world-class thrower can get the hammer up to a speed of 29 m/s. If an athlete swings the mass in a horizontal circle centered on the handle he uses to hold the chain, what is the tension in the chain?

In the hammer throw, an athlete spins a heavy mass in a circle at the end of a chain, then lets go of the chain. For male athletes, the “hammer” is a mass of 7.3 kg at the end of a 1.2 m chain.

Slide 6-29

𝑚 𝑣2

𝑟

𝑇=𝑚 𝑣2

𝑟=7.3kg

(29ms )

2

1.2m

Problem solving uniform circular motion

Page 22: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car of mass 1500 kg goes over a hill at a speed of 20 m/s. The shape of the hill is approximately circular, with a radius of 60 m, as in the figure at right. When the car is at the highest point of the hill,

a. What is the force of gravity on the car?

b. What is the normal force of the road on the car at this point?

Slide 6-30

Problem solving uniform circular motion

𝐹=𝑚𝑔

Page 23: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car of mass 1500 kg goes over a hill at a speed of 20 m/s. The shape of the hill is approximately circular, with a radius of 60 m, as in the figure at right. When the car is at the highest point of the hill,

a. What is the force of gravity on the car?

b. What is the normal force of the road on the car at this point?

Slide 6-30

Problem solving uniform circular motion

∑ 𝐹 𝑦=¿𝑁+𝑚𝑔=−𝑚 𝑣2

𝑟¿

𝑁=−𝑚 (𝑣2

𝑟+𝑔)

Page 24: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

vmax gr

Slide 6-31

Maximum walking speed

Page 25: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A roller coaster car goes through a vertical loop at a constant speed. For positions A to E, rank order the:

• centripetal acceleration

• normal force

• apparent weight

Slide 6-32

Example Problem

𝑎=𝑣2

𝑟

A = B = C = D = E

Page 26: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A roller coaster car goes through a vertical loop at a constant speed. For positions A to E, rank order the:

• centripetal acceleration

• normal force

• apparent weight

Slide 6-32

Example Problem

A = E > B = D > C

Page 27: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A roller coaster car goes through a vertical loop at a constant speed. For positions A to E, rank order the:

• centripetal acceleration

• normal force

• apparent weight

Slide 6-32

Example Problem

A = E > B = D > C

Page 28: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Net Force causes centripetal acceleration

∑ 𝐹=𝐹 net

Page 29: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Net Force causes centripetal acceleration

Page 30: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Friction force as a Net Force

Page 31: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Problem solving circular motion with Net Force

𝑓 𝑠=𝜇𝑠𝑚𝑐𝑔¿𝑚𝑐𝑣2

𝑟𝑣=√𝜇𝑠𝑔𝑟

Page 32: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car travels around a corner with the cruise control on. Which vector is the car’s centripetal acceleration?

A. AB. BC. CD. DE. E

A B C D E

0% 2%

94%

2%2%

Page 33: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car travels around a corner while speeding up. Which vector is the net force on the car?

A. AB. BC. CD. DE. E

A B C D E

0% 2%

84%

6%8%

Page 34: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car travels around a corner while speeding up. Which vector is the force of friction from the road on the car?

A. AB. BC. CD. DE. E

A B C D E

2% 0% 2%

96%

0%

Page 35: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Fictitious Forces in circular motion

Feels like something is pushing you out of the

car

Page 36: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A car travels around a corner at a constant speed. Which vector is the fictitious force on the car?

A. AB. BC. CD. DE. E

A B C D E

0%

100%

0%0%0%

Page 37: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

This one guy you knew from a while back says that in order to avoid loss of bone density on his trip to mars so, the ship must be spinning to simulate gravity. How fast must the craft below spin to simulate gravity?

𝑁

𝑣𝐹 𝑔=𝑁

𝑚𝑔=𝑚 𝑣2

𝑟

𝑣=√𝑔𝑟

Simulating Gravity

Page 38: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Tilted roads in favor of circular motion

Page 39: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Example Problem: Over the TopA handful of professional skaters have taken a skateboard through an inverted loop in a full pipe. For a typical pipe with diameter 14 ft, what is the minimum speed the skater must have at the very top of the loop?

Slide 6-33

Page 40: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Example Problem: Over the TopA handful of professional skaters have taken a skateboard through an inverted loop in a full pipe. For a typical pipe with diameter 14 ft, what is the minimum speed the skater must have at the very top of the loop?

Slide 6-33

𝐹 𝑔

𝑁=0∑ 𝐹=𝐹𝑔=𝑚𝑣2

𝑟−𝑚𝑔=−𝑚𝑣2

𝑟

𝑣=√|𝑔|𝑟

help: |𝑔|=32ft

s2

Page 41: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Keeping riders safe in circular motion

Page 42: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

When a ball on the end of a string is swung in a vertical circle, the ball’s acceleration is because

A. The speed is changingB. The direction is changingC. The speed and direction are

changingD. The ball is not acceleration

The s

peed is

changin

g

The d

irecti

on is ch

angin

g

The s

peed an

d directi

on are...

The b

all is

not acce

leration

0% 0%0%

100%

Page 43: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Slide 6-35

The Force of Gravity

Page 44: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

𝑦

𝑥

Same as the familiar y and x

The inverse-square law

Page 45: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

versus in Newton’s law of gravitation

is a value unique to the mass that’s pulling

is the same throughout the whole universe!

Page 46: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A typical bowling ball is spherical, weighs 16 pounds, and has a diameter of 8.5 in. Suppose two bowling balls are right next to each other in the rack. What is the gravitational force between the two—magnitude and direction? What is the magnitude and direction of the force of gravity on a 60 kg person?

Example Problem

Slide 6-36

Page 47: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A 60 kg person stands on each of the following planets. Ranks order her weight on the three

bodies, from highest to lowest

A. A>B>CB. B>A>CC. B>C>AD. C>B>AE. C>A>B

A>B>C

B>A>C

B>C>AC>B

>AC>A

>B

77%

0% 0%

19%

4%

Page 48: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Which vector pair matches the car’s motion over the hill?

A. AB. BC. C

A B C

94%

2%4%

Page 49: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

Page 50: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

© 2015 Pearson Education, Inc.

The Force of Gravity

𝑣=√𝐺𝑀 e

𝑟 e

17,000 mph

Page 51: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Example Problem: Orbital MotionPhobos is one of two small moons that orbit Mars. Phobos is a very small moon, and has correspondingly small gravity—it varies, but a typical value is about 6 mm/s2. Phobos isn’t quite round, but it has an average radius of about 11 km. What would be the orbital speed around Phobos, assuming it was round with gravity and radius as noted?

Slide 6-34

𝑣=√𝐺𝑀𝑟 e

=√ (6.67 ∙ 10−11 𝑚3

kg ∙ s2 )( .0069.8

∙ 5.97 ∙1024 kg )6.4 ∙106 m

Page 52: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

A satellite orbits the earth. A space shuttle crew is sent to boost the satellite into a higher orbit.

Which of these quantities increases?

A. SpeedB. Angular speedC. PeriodD. Centripetal accelerationE. Gravitational force of the

earth Speed

Angular

speed

Period

Centripet

al ac

celerati

on

Gravita

tional fo

rce of t

he earth

0% 2% 0%4%

94%

Page 53: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Summary

Slide 6-41

Page 54: Chapter 6 Circular Motion, Orbits, and Gravity. Slide 6-23 Uniform Circular Motion.

Summary

Slide 6-42