Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics...

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Chapter 11A – Angular Motion Chapter 11A – Angular Motion A PowerPoint Presentation by A PowerPoint Presentation by Paul E. Tippens, Professor Paul E. Tippens, Professor of Physics of Physics Southern Polytechnic State Southern Polytechnic State University University © 2007

Transcript of Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics...

Page 1: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Chapter 11A – Angular MotionChapter 11A – Angular Motion

A PowerPoint Presentation byA PowerPoint Presentation by

Paul E. Tippens, Professor of Paul E. Tippens, Professor of PhysicsPhysics

Southern Polytechnic State Southern Polytechnic State UniversityUniversity

A PowerPoint Presentation byA PowerPoint Presentation by

Paul E. Tippens, Professor of Paul E. Tippens, Professor of PhysicsPhysics

Southern Polytechnic State Southern Polytechnic State UniversityUniversity© 2007

Page 2: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

WIND TURBINES such as these can generate significant energy in a way that is environ-mentally friendly and renewable. The concepts of rotational acceleration, angular velocity, angular displacement, rotational inertia, and other topics discussed in this chapter are useful in describing the operation of wind turbines.

Page 3: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Objectives: After completing Objectives: After completing this module, you should be this module, you should be able to:able to:• Define and apply concepts of angular Define and apply concepts of angular

displacement, velocity, and displacement, velocity, and acceleration.acceleration.

• Draw analogies relating rotational-Draw analogies relating rotational-motion parameters (motion parameters (, , , , ) to linear ) to linear ((x, v, ax, v, a) and solve rotational problems.) and solve rotational problems.

• Write and apply relationships between Write and apply relationships between linear and angular parameters.linear and angular parameters.

Page 4: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Objectives: (Continued)Objectives: (Continued)

• Define moment of inertia and apply it for several regular objects in Define moment of inertia and apply it for several regular objects in rotation.rotation.

• Apply the following concepts to rotation:Apply the following concepts to rotation:

1. Rotational work, energy, and power1. Rotational work, energy, and power

2. Rotational kinetic energy and 2. Rotational kinetic energy and momentummomentum

3. Conservation of angular momentum3. Conservation of angular momentum

Page 5: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Rotational Displacement, Rotational Displacement,

Consider a disk that rotates from A to Consider a disk that rotates from A to B:B:

A

B

Angular displacement Angular displacement ::

Measured in Measured in revolutions, degrees, or revolutions, degrees, or

radians.radians.

1 rev1 rev == 360 360 00 = 2= 2 radrad

The best measure for rotation of The best measure for rotation of rigid bodies is the rigid bodies is the radianradian..

The best measure for rotation of The best measure for rotation of rigid bodies is the rigid bodies is the radianradian..

Page 6: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Definition of the RadianDefinition of the RadianOne One radian radian is the angle is the angle subtended at the center of a circle subtended at the center of a circle by an arc length by an arc length ss equal to the equal to the radius radius RR of the circle. of the circle.

1 rad = = 57.30

R

R

ss

R

s

R

Page 7: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 1:Example 1: A rope is wrapped many A rope is wrapped many times around a drum of radius times around a drum of radius 50 cm50 cm. . How many revolutions of the drum are How many revolutions of the drum are required to raise a bucket to a height required to raise a bucket to a height of of 20 m20 m??

h = h = 20 m20 m

RR= 40 rad= 40 rad

Now, Now, 1 rev = 21 rev = 2 radrad

= 6.37 rev = 6.37 rev

1 rev40 rad

2 rad

20 m

0.50 m

s

R

Page 8: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 2:Example 2: A bicycle tire has a A bicycle tire has a radius of radius of 25 cm25 cm. If the wheel makes . If the wheel makes 400 rev400 rev, how far will the bike have , how far will the bike have traveled?traveled?

= 2513 rad= 2513 rad

s = s = R = R = 25132513 rad (0.25 m)rad (0.25 m)

s = 628 ms = 628 m

2 rad400 rev

1 rev

Page 9: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular VelocityAngular VelocityAngular velocityAngular velocity,, is the rate of is the rate of change in angular displacement. change in angular displacement. (radians per second.)(radians per second.)

ff Angular frequency Angular frequency ff (rev/s).(rev/s).ff Angular frequency Angular frequency ff (rev/s).(rev/s).

Angular velocity can also be given as Angular velocity can also be given as the frequency of revolution, the frequency of revolution, f f (rev/s or (rev/s or rpm):rpm):

Angular velocity Angular velocity in rad/s.in rad/s.

tt

Page 10: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 3:Example 3: A rope is wrapped many A rope is wrapped many times around a drum of radius times around a drum of radius 20 cm20 cm. . What is the angular velocity of the What is the angular velocity of the drum if it lifts the bucket to drum if it lifts the bucket to 10 m10 m in in 5 5 ss??

h = h = 10 m10 m

R

= 10.0 rad/s = 10.0 rad/s

t

50 rad

5 s

= 50 rad= 50 rad10 m

0.20 m

s

R

Page 11: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 4:Example 4: In the previous example, In the previous example, what is the frequency of revolution for what is the frequency of revolution for the drum? Recall that the drum? Recall that = 10.0 rad/s = 10.0 rad/s..

h = 10 mh = 10 m

R

f = 95.5 rpmf = 95.5 rpm

2 or 2

f f

10.0 rad/s1.59 rev/s

2 rad/revf

Or, since 60 s = 1 min:Or, since 60 s = 1 min:

rev 60 s rev1.59 95.5

1 min minf

s

Page 12: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular AccelerationAngular AccelerationAngular accelerationAngular acceleration is the rate of is the rate of

change in angular velocity. (Radians per change in angular velocity. (Radians per sec per sec.)sec per sec.)

The angular acceleration can also be The angular acceleration can also be found from the change in frequency, as found from the change in frequency, as follows:follows:

2 ( ) 2

fSince f

t

2 ( ) 2

fSince f

t

2 Angular acceleration (rad/s )t

2 Angular acceleration (rad/s )

t

Page 13: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 5:Example 5: The block is lifted from The block is lifted from rest until the angular velocity of the rest until the angular velocity of the drum is drum is 1616 rad/srad/s after a time of after a time of 4 s4 s. . What is the average angular What is the average angular acceleration?acceleration?

h = h = 20 m20 m

R

= 4.00 rad/s2 = 4.00 rad/s2

0

f o fort t

2

16 rad/s rad4.00

4 s s

Page 14: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular and Linear SpeedAngular and Linear SpeedFrom the definition of angular

displacement:s = R Linear vs. angular

displacement

v = Rs R

v Rt t t

Linear speed = angular speed x radius

Linear speed = angular speed x radius

Page 15: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular and Linear Angular and Linear Acceleration:Acceleration:

From the velocity relationship we have:

v = R Linear vs. angular velocity

a = Rv v R v

v Rt t t

Linear accel. = angular accel. x radius

Linear accel. = angular accel. x radius

Page 16: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Examples:Examples:

R1 = 20 cm R2 = 40 cm

R1

R2

A

B = 0; f = 20 rad/s

t = 4 s What is final linear

speed at points A and B?

Consider flat rotating Consider flat rotating disk:disk:

vAf = Af R1 = (20 rad/s)(0.2 m); vvAfAf = 4= 4 m/sm/s

vAf = Bf R1 = (20 rad/s)(0.4 m); vvBfBf = 8= 8 m/sm/s

Page 17: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Acceleration ExampleAcceleration Example

R1 = 20 cm R2 = 40 cm

What is the What is the averageaverage angular and linear angular and linear acceleration at B?acceleration at B?

R1

R2

A

B = 0; f = 20 rad/s t = 4 s

Consider flat rotating Consider flat rotating disk:disk:

= 5.00 rad/s2= 5.00 rad/s2

a = R = (5 rad/s2)(0.4 m) a= 2.00 m/s2a= 2.00 m/s2

0 20 rad/s

4 sf

t

Page 18: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular vs. Linear ParametersAngular vs. Linear Parameters

Angular accelerationAngular acceleration is the time is the time rate of change in angular velocity.rate of change in angular velocity.

0f

t

0f

t

Recall the definition of Recall the definition of linear acceleration linear acceleration aa from from kinematicskinematics..

0fv va

t

0fv va

t

But, But, aa = = RR and and vv = = RR, so that we may , so that we may write:write:

0fv va

t

becom

es

0fR RR

t

Page 19: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

A Comparison: Linear vs. AngularA Comparison: Linear vs. Angular

0

2fv v

s vt t

0

2fv v

s vt t

0

2ft t

0

2ft t

f o t f o t f ov v at f ov v at

210 2t t 21

0 2t t 210 2s v t at 21

0 2s v t at

212f t t 21

2f t t

2 202 f 2 2

02 f 2 202 fas v v 2 2

02 fas v v

212fs v t at 21

2fs v t at

Page 20: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Linear Example:Linear Example: A car traveling A car traveling initially at initially at 20 m/s20 m/s comes to a stop in comes to a stop in a distance of a distance of 100 m100 m. What was the . What was the acceleration?acceleration?

100 100 mm

vvoo = 20 = 20 m/sm/s

vvff = 0 = 0 m/sm/s

Select Equation:

2 202 fas v v

a = = 0 - vo

2

2s

-(20 m/s)2

2(100 m) a = -2.00 m/s2a = -2.00 m/s2

Page 21: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Angular analogy:Angular analogy: A disk (R = 50 cm), rotating at 600 rev/min comes to a stop after making 50 rev. What is the acceleration?

Select Equation:

2 202 f

= = 0 - o

2

2

-(62.8 rad/s)2

2(314 rad) = -6.29 m/s2 = -6.29 m/s2

Ro = 600 rpm

f = 0 rpm

= 50 rev

2 rad 1 min600 62.8 rad/s

min 1 rev 60 s

rev

50 rev = 314 rad

Page 22: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Problem Solving Strategy:Problem Solving Strategy: Draw and label sketch of problem.Draw and label sketch of problem.

Indicate Indicate ++ direction of rotation. direction of rotation.

List givens and state what is to be found.List givens and state what is to be found.

Given: ____, _____, _____ (,,f,,t)

Find: ____, _____ Select equation containing one and

not the other of the unknown quantities, and solve for the unknown.

Page 23: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Example 6:Example 6: A drum is rotating clockwise A drum is rotating clockwise initially at initially at 100 rpm100 rpm and undergoes a and undergoes a constant counterclockwise acceleration constant counterclockwise acceleration of of 3 rad/s3 rad/s22 for for 2 s2 s. What is the angular . What is the angular displacement?displacement?

= -14.9 rad = -14.9 rad

Given:Given: o = -100 rpm; t = 2 s = +2 rad/s2

2 21 12 2( 10.5)(2) (3)(2)ot t

rev 1 min 2 rad100 10.5 rad/s

min 60 s 1 rev

= -20.9 rad + 6 rad

Net displacement is clockwise (-)

R

Page 24: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

Summary of Formulas for RotationSummary of Formulas for Rotation

0

2fv v

s vt t

0

2fv v

s vt t

0

2ft t

0

2ft t

f o t f o t f ov v at f ov v at

210 2t t 21

0 2t t 210 2s v t at 21

0 2s v t at

212f t t 21

2f t t

2 202 f 2 2

02 f 2 202 fas v v 2 2

02 fas v v

212fs v t at 21

2fs v t at

Page 25: Chapter 11A – Angular Motion A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University A PowerPoint Presentation.

CONCLUSION: Chapter 11A CONCLUSION: Chapter 11A Angular MotionAngular Motion