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Chapter 7 Rotational Motion
44

Chapter 7

Jan 23, 2016

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Chapter 7. Rotational Motion. The Radian. The radian is a unit of angular measure The radian can be defined as the arc length s along a circle divided by the radius r. More About Radians. Comparing degrees and radians Converting from degrees to radians. Angular Displacement. - PowerPoint PPT Presentation
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Transcript
Page 1: Chapter 7

Chapter 7

Rotational Motion

Page 2: Chapter 7

The Radian

The radian is a unit of angular measure

The radian can be defined as the arc length s along a circle divided by the radius r

sr

Page 3: Chapter 7

More About Radians

Comparing degrees and radians

Converting from degrees to radians

3.572

360rad1

]rees[deg180

]rad[

Page 4: Chapter 7

Angular Displacement

Axis of rotation is the center of the disk

Need a fixed reference line

During time t, the reference line moves through angle θ

Page 5: Chapter 7

Rigid Body

Every point on the object undergoes circular motion about the point O

All parts of the object of the body rotate through the same angle during the same time

The object is considered to be a rigid body This means that each part of the body is fixed in

position relative to all other parts of the body

Page 6: Chapter 7

Angular Displacement, cont.

The angular displacement is defined as the angle the object rotates through during some time interval

The unit of angular displacement is the radian Each point on the object undergoes the same

angular displacement

fi

Page 7: Chapter 7

Average Angular Speed

The average angular speed, ω, of a rotating rigid object is the ratio of the angular displacement to the time interval

fiav

fit t t

Page 8: Chapter 7

Angular Speed, cont.

The instantaneous angular speed is defined as the limit of the average speed as the time interval approaches zero

Units of angular speed are radians/sec rad/s

Speed will be positive if θ is increasing (counterclockwise)

Speed will be negative if θ is decreasing (clockwise)

Page 9: Chapter 7

Average Angular Acceleration

The average angular acceleration, , of an object is defined as the ratio of the change in the angular speed to the time it takes for the object to undergo the change:

fiav

fit t t

Page 10: Chapter 7

Angular Acceleration, cont

Units of angular acceleration are rad/s² Positive angular accelerations are in the

counterclockwise direction and negative accelerations are in the clockwise direction

When a rigid object rotates about a fixed axis, every portion of the object has the same angular speed and the same angular acceleration

Page 11: Chapter 7

Angular Acceleration, final

The sign of the acceleration does not have to be the same as the sign of the angular speed

The instantaneous angular acceleration is defined as the limit of the average acceleration as the time interval approaches zero

Page 12: Chapter 7

Analogies Between Linear and Rotational Motion

Page 13: Chapter 7

Relationship Between Angular and Linear Quantities

Displacements

Speeds

Accelerations

Every point on the rotating object has the same angular motion

Every point on the rotating object does not have the same linear motion

rs

tv r

ta r

Page 14: Chapter 7

Centripetal Acceleration

An object traveling in a circle, even though it moves with a constant speed, will have an acceleration

The centripetal acceleration is due to the change in the direction of the velocity

Page 15: Chapter 7

Centripetal Acceleration, cont.

Centripetal refers to “center-seeking”

The direction of the velocity changes

The acceleration is directed toward the center of the circle of motion

Page 16: Chapter 7

Centripetal Acceleration, final

The magnitude of the centripetal acceleration is given by

This direction is toward the center of the circle

2

c

va

r

Page 17: Chapter 7

Centripetal Acceleration and Angular Velocity

The angular velocity and the linear velocity are related (v = ωr)

The centripetal acceleration can also be related to the angular velocity

ra 2C

Page 18: Chapter 7

Total Acceleration

The tangential component of the acceleration is due to changing speed

The centripetal component of the acceleration is due to changing direction

Total acceleration can be found from these components

2C

2t aaa

Page 19: Chapter 7

Vector Nature of Angular Quantities

Angular displacement, velocity and acceleration are all vector quantities

Direction can be more completely defined by using the right hand rule

Grasp the axis of rotation with your right hand

Wrap your fingers in the direction of rotation

Your thumb points in the direction of ω

Page 20: Chapter 7

Velocity Directions, Example

In a, the disk rotates clockwise, the velocity is into the page

In b, the disk rotates counterclockwise, the velocity is out of the page

Page 21: Chapter 7

Acceleration Directions

If the angular acceleration and the angular velocity are in the same direction, the angular speed will increase with time

If the angular acceleration and the angular velocity are in opposite directions, the angular speed will decrease with time

Page 22: Chapter 7

Forces Causing Centripetal Acceleration

Newton’s Second Law says that the centripetal acceleration is accompanied by a force FC = maC

FC stands for any force that keeps an object following a circular path Tension in a string Gravity Force of friction

Page 23: Chapter 7

Reading Quiz

1. For uniform circular motion, the acceleration

A. is parallel to the velocity.B. is directed toward the center of the circle.C. is larger for a larger orbit at the same speed.D. is always due to gravity.E. is always negative.

Page 24: Chapter 7

Answer

1. For uniform circular motion, the acceleration

A. is parallel to the velocity.B. is directed toward the center of the circle.C. is larger for a larger orbit at the same speed.D. is always due to gravity.E. is always negative.

Slide 6-7

Page 25: Chapter 7

Problem Solving Strategy

Draw a free body diagram, showing and labeling all the forces acting on the object(s)

Choose a coordinate system that has one axis perpendicular to the circular path and the other axis tangent to the circular path The normal to the plane of motion is also often

needed

Page 26: Chapter 7

Problem Solving Strategy, cont.

Find the net force toward the center of the circular path (this is the force that causes the centripetal acceleration, FC)

Use Newton’s second law The directions will be radial, normal, and tangential The acceleration in the radial direction will be the

centripetal acceleration

Solve for the unknown(s)

Page 27: Chapter 7

Applications of Forces Causing Centripetal Acceleration

Many specific situations will use forces that cause centripetal acceleration Level curves Banked curves Horizontal circles Vertical circles

Page 28: Chapter 7

Level Curves

Friction is the force that produces the centripetal acceleration

Can find the frictional force, µ, or v

rgv

Page 29: Chapter 7

Motion on a Flat Curve

Page 30: Chapter 7

Banked Curves

A component of the normal force adds to the frictional force to allow higher speeds

2

tan

tanc

vrg

or a g

Page 31: Chapter 7

Motion on a Banked Curve

Page 32: Chapter 7

Reading Quiz

2. When a car turns a corner on a level road, which force provides the necessary centripetal acceleration?

A. Friction B. TensionC. Normal forceD. Air resistanceE. Gravity

Page 33: Chapter 7

Answer

2. When a car turns a corner on a level road, which force provides the necessary centripetal acceleration?

A. Friction B. TensionC. Normal forceD. Air resistanceE. Gravity

Slide 6-9

Page 34: Chapter 7

Vertical Circle

Look at the forces at the top of the circle

The minimum speed at the top of the circle can be found

gRv top

Page 35: Chapter 7

Loop de Loop

Page 36: Chapter 7

Forces in Accelerating Reference Frames

Distinguish real forces from fictitious forces “Centrifugal” force is a fictitious force Real forces always represent interactions

between objects

Page 37: Chapter 7

When a ball on the end of a string is swung in a vertical circle, the ball is accelerating because

A. the speed is changing.B. the direction is changing.C. the speed and the direction are changing.D. the ball is not accelerating.

Checking Understanding

Page 38: Chapter 7

Answer

When a ball on the end of a string is swung in a vertical circle, the ball is accelerating because

A. the speed is changing.B. the direction is changing.C. the speed and the direction are changing.D. the ball is not accelerating.

Page 39: Chapter 7

When a ball on the end of a string is swung in a vertical circle:What is the direction of the acceleration of the ball?

A. Tangent to the circle, in the direction of the ball’s motion

B. Toward the center of the circle

Checking Understanding

Page 40: Chapter 7

Answer

When a ball on the end of a string is swung in a vertical circle:What is the direction of the acceleration of the ball?

A. Tangent to the circle, in the direction of the ball’s motion

B. Toward the center of the circle

Page 41: Chapter 7

For the ball on the end of a string moving in a vertical circle:What force is producing the centripetal acceleration of the ball?

A. gravityB. air resistanceC. normal forceD. tension in the string

Checking Understanding:Circular Motion Dynamics

Page 42: Chapter 7

Answer

For the ball on the end of a string moving in a vertical circle:What force is producing the centripetal acceleration of the ball?

A. gravityB. air resistanceC. normal forceD. tension in the string

Page 43: Chapter 7

For the ball on the end of a string moving in a vertical circle:What is the direction of the net force on the ball?

A. tangent to the circleB. toward the center of the circleC. there is no net force

Checking Understanding:Circular Motion Dynamics

Page 44: Chapter 7

Answer

For the ball on the end of a string moving in a vertical circle:What is the direction of the net force on the ball?

A. tangent to the circleB. toward the center of the circleC. there is no net force

Slide 6-20