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Physics 218, Lecture XX 1 Physics 218 Lecture 20 Dr. David Toback

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Page 1: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 1

Physics 218Lecture 20 Dr. David Toback

Page 2: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 2

Angular Quantities

• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:

– Mass

– Momentum

– Energy

Page 3: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 3

Page 4: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 4

Angular Quantities

• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:

– Mass

– Momentum

– Energy

Page 5: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 5

Calculating Moments of Inertia

dmR I

mR I

2

2

Page 6: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 6

Calculate the Moment of Inertia

A pulley has mass M, uniform density, radius R, and rotates around its fixed axis

Calculate its moment of inertia

R

Page 7: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 7

Angular Quantities

• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:

– Mass Moment of Inertia – Momentum

– Energy

Page 8: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 8

Angular Momentum

Define the Angular Momentum L

L = I

Is this a vector?

dt

dLI

dt

dL

dt

Ld

dt

Id

dt

dII

)()(

Page 9: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 9

Newton’s Laws

• Momentum vs. Angular Momentum

p=mv L=I

• Newton’s Laws

F=dp/dt = dL/dt

Page 10: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 10

Conservation of Angular Momentum

Const L 0 if

dt

dL

By Newton’s laws, the angular momentum of a body can change, but the angular momentum for a system cannot

change Conservation of Angular Momentum

Page 11: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 11

Ice Skater

• This one you’ve seen on TV

• Try this at home in a chair that rotates

• Get yourself spinning with your arms and legs stretched out, then pull them in

Page 12: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 12

Clutch Design

Model a car clutch as two plates, each with radius R, and masses MA and MB

Assume IPlate = ½MR2

Plate A spins with speed 1 and Plate B is at rest.

We close them and they spin together

Find the final angular velocity of the system

Page 13: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 13

Angular Quantities

• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:

– Mass Moment of Inertia – Momentum Angular Momentum L

– Energy

Page 14: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 14

Rotational Kinetic Energy

KE = ½I2

Conservation of Energy must take into account

rotational kinetic energy

Page 15: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 15

Rotating Rod

A rod of mass uniform density, mass m and length l pivots at a hinge. It starts at rest at a right angle and is let go

What is when it reaches the bottom?

What is the velocity of the tip at the bottom?

Page 16: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 16

Rotation and Translation• Objects can both Rotate

and Translate

• Both have energy separately

KE = ½ mv2 + ½I2

• Always true when you have rolling without slipping

Page 17: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 17

Rolling Down an Incline

A solid ball of mass m and radius R rolls without slipping down a plane with height h.

What will be the final speed of the ball?

What would be the speed if the ball didn’t roll? Note:

Isphere = 2/5MR2

Page 18: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 18

Person on a Disk

A person with mass m stands on the edge of a disk with radius R and moment ½MR2. Neither is moving.

The person then starts moving on the disk with speed V.

Find the angular velocity of the disk

Page 19: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 19

Same Problem: Forces

Same problem but with Forces

Page 20: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 20

Next Time

• Chapter 11– It’s a review of Chapter 10, but more

sophisticated

– Math, Torque, Angular Momentum, Energy

• The material will not be on the 3rd exam, but will help with the exam. It will all be on the final.

• Exam 3 is Tuesday November 26th

Page 21: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 21

Page 22: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 22

Hollow Cylinder

Consider a hollow cylinder with uniform density, inner radius R1, outer radius R2 and total Mass M.

Find the moment of Inertia

Page 23: Physics 218, Lecture XX1 Physics 218 Lecture 20 Dr. David Toback

Physics 218, Lecture XX 23

Parallel-Axis Theorem

• Quick Trick for calculating Moments

• I = Icm + Mh2

• Example