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Physics 215 – Fall 2014 Lecture 11-2 1 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

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Page 1: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 1

Welcome back to Physics 215

Today’s agenda:

• Angular Momentum

• Rolling

Page 2: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 2

Current homework assignment

• HW9:– Knight Textbook Ch.12: 74, 80, 82, 86– 2 exam-style web problems

Page 3: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 3

Angular Momentum

• can define rotational analog of linear

momentum called angular momentum

• in absence of external torque it will be

conserved in time

• True even in situations where Newton’s laws fail ….

Page 4: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 4

Definition of Angular Momentum

* Back to slide on rotational dynamics:miri

2/t = i

* Rewrite, using li = miri2

li/t = i

* Summing over all particles in body:

L/t = ext

L = angular momentum = I

pivot

ri

mi

Fi

Page 5: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 5

An ice skater spins about a vertical axis through her body with her arms held out. As she draws her arms in, her angular velocity

• 1. increases• 2. decreases• 3. remains the same• 4. need more information

Page 6: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 6

Angular Momentum 1.

p

r

O

Point particle:|L| = |r||p|sin() = m|r||v| sin()

vector form L = r x p – direction of L given by right hand rule

(into paper here)

L = mvr if v is at 900 to r for single particle

Page 7: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 7

Angular Momentum 2.

o

rigid body:* |L| = I fixed axis of rotation)* direction – along axis – into paper here

Page 8: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 8

Rotational Dynamics

L/t =

These are equivalent statements

If no net external torque: * L is constant in time * Conservation of Angular Momentum * Internal forces/torques do not contribute to external torque.

Page 9: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 9

Bicycle wheel demo

• Spin wheel, then step onto platform

• Apply force to tilt axle of wheel

Page 10: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 10

Linear and rotational motion

• Force

• Acceleration

• Momentum

Kinetic energy

• Torque

• Angular acceleration

• Angular momentum

• Kinetic energy

*rotations about fixed pivot or symmetry axis

Page 11: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 11

A hammer is held horizontally and then released. Which way will it fall?

Page 12: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 12

General motion of extended objects

• Net force acceleration of CM

• Net torque about CM angular acceleration

(rotation) about CM

• Resultant motion is superposition of these two motions

• Total kinetic energy K = KCM + Krot

Page 13: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 13

1. A.

2. B.

3. C.

4. A and C.

Three identical rectangular blocks are at rest on a flat, frictionless table. The same force is exerted on each of the three blocks for a very short time interval. The force is exerted at a different point on each block, as shown.

After the force has stopped acting on each block, which block will spin the fastest?

Top-view diagram

Page 14: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 14

1. A.2. B.3. C.4. A, B, and C have the same C.O.M. speed.

Three identical rectangular blocks are at rest on a flat, frictionless table. The same force is exerted on each of the three blocks for a very short time interval. The force is exerted at a different point on each block, as shown.

After each force has stopped acting, which block’s center of mass will have the greatest speed?

Top-view diagram

Page 15: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 15

Rolling without slipping

translation rotation

vcm =

acm =

Page 16: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 16

Rolling without slipping

N

W

F

F = maCM

= I

Now aCM = R if no slipping

So, m aCM

and F =

Page 17: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 17

A ribbon is wound up on a spool. A person pulls the ribbon as shown.

Will the spool move to the left, to the right, or will it not move at all?

1. The spool will move to the left.

2. The spool will move to the right.

3. The spool will not move at all.

Page 18: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 18

1. The spool will move to the left.

2. The spool will move to the right.

3. The spool will not move at all.

A ribbon is wound up on a spool. A person pulls the ribbon as shown.

Will the spool move to the left, to the right, or will it not move at all?

Page 19: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 19

A ribbon is wound up on a spool. A person pulls the ribbon as shown.

Will the spool move to the left, to the right, or will it not move at all?

1. The spool will move to the left.

2. The spool will move to the right.

3. The spool will not move at all.

Page 20: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 20

Page 21: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 21

Page 22: Physics 215 – Fall 2014Lecture 11-21 Welcome back to Physics 215 Today’s agenda: Angular Momentum Rolling

Physics 215 – Fall 2014 Lecture 11-2 22

Reading assignment

• Gravitation -- Ch. 13 in textbook