physics 7b lecture 824-feb-2010 slide 1 of 31 physics 7b-1 (a/b) professor cebra rotational...

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Physics 7B Lecture 8 24-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture 8

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Page 1: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 1 of 31

Physics 7B-1 (A/B)Professor Cebra

Rotational Kinematics and Angular Momentum

Conservation

Winter 2010Lecture 8

Page 2: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 2 of 31

Rotational Motion

If the force is always perpendicular to the direction of the velocity, then only the direction changes.

Centripetal Acceleration

v = 2pr/T

r

v

t

va

r

tv

v

v

c

2

Centripetal Force

Fc = mac=mv2/r

FC

Page 3: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 3 of 31

Angular Quantities• There is an analogy between objects moving along a straight path

and objects moving along a circular path.

Linear RotationalPosition (x) ↔ Angle (q)Velocity (v) ↔ Angular Velocity (w)

Acceleration (a) ↔ Angular Acceleration (a)Momentum (p) ↔ Angular Momentum (L)

Force (F) ↔ Torque (t)Mass (m) ↔ Moment of Inertia (I)

Page 4: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 4 of 31

Angular Displacement

q

By convention, q is measured clockwise from the x-axis.

Page 5: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 5 of 31

Angular Velocity

• Angular velocity is a vector:– Right hand rule to determines direction of ω

– Velocity and radius determine magnitude of ω

r

vtvt

r

Page 6: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 6 of 31

Angular Velocity

• What’s the angular velocity of a point particle?

sinr

v

r

v

v

r┴

r

θ

Page 7: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 7 of 31

Angular Acceleration

• Angular Acceleration: Rate of change in angular velocity

• A stationary disk begins to rotate. After 3 seconds, it is rotating at 60 rad/sec. What is the average angular acceleration?

r

a

dt

d t

2s

rad

s

rad/s rad/s

t20

3

060

Page 8: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 8 of 31

Rotational Kinematics

Rotational Motion(a = constant)

Linear Motion(a = constant)

= w w0 + at v = v0 + at

q = (1/2)(w0 + w)t x = (1/2)(v0 + v)t

q = q0 + w0t + (1/2)at2 x = x0 + v0t + (1/2)at2

w2 = w02 + 2aq v2 = v0

2 + 2ax

Page 9: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 9 of 31

Rotational Kinematics

A commercial jet airplane is idling at the end of the run way. At idle, the turbo fans are rotating with an angular velocity of 175 rad/sec. The Tower gives the jetliner permission to take-off. The pilot winds up the jet engines with an angular acceleration of 175 rad/s2. The engines wind up through an angular displacement of 2000 radians. What is the final angular velocity of the turbo-fan blades?

Solution:w2 = w0

2 + 2aq = (175 rad/s)2 + 2(175 rad/s2)(2000 rad) = 7.00 x 105 rad2/s2

w = 837 rad/s

Page 10: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 10 of 31

Angular Momentum

• What’s the momentum of a rolling disk?

• Two types of motion:

– Translation:

– Rotation:

v

vmp disk

diskIL

Page 11: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 11 of 31

Angular Momentum

• Angular Momentum: Product of position vector and momentum vector

• Why is angular momentum important? Like energy and momentum, angular momentum is conserved.

12 LLL

sinrpprL

• Angular Impulse: Change in angular momentum vector

Page 12: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 12 of 31

Angular Momentum

• What’s the angular momentum of a point particle?

p rprL sin

p

r┴

r

θ

Page 13: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 13 of 31

Torque

• Which way will the scale tip?

• Rotation of scale is influenced by:– Magnitude of forces– Location of forces

1 kg 1.5 kg 1 kg 1.5 kg

Page 14: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 14 of 31

Torque

• Which is more effective?

• Rotation of wrench is influenced by:– Magnitude of forces– Location of forces– Direction of forces

F1 F2F1

F2

DEMO: Torque Meter

Page 15: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 15 of 31

Torque

• Torque: The cause or agent of angular acceleration

• The angular velocity of an object will not change unless acted upon by a torque

• The net torque on an object is equal to the rate of change of angular momentum

00 Object on Net

dt

LdObject on Net

sinrFFr

Page 16: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 16 of 31

Newton’s Second Law - Rotation

t = Ia

Idt

dI

dt

dI

dt

LdObjectonNet

Angular impulse = tDt = DL

Page 17: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 17 of 31

Torque

• What’s the torque on a point particle?

F rFr sin

F

r┴

r

θ

Page 18: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 18 of 31

Rotational Kinetic Energy

• What’s the kinetic energy of a rolling disk?

• Two types of motion:

– Translation:

– Rotation:

v

2

2

1vmKE disktran

2

2

1 diskrot IKE

Page 19: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 19 of 31

Rolling Bodies

mg

q

Normal Force:FN = mg cosq

Parallel Force:FP = mg sinq

Frictional Force:f < msFN = msmg cosq

Angular Accelerationt= I a t = fR

Linear AccelerationFtot = maFtot = mg sinq – f

a = a/R

Page 20: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 20 of 31

Moment of Inertia

Demo: Crazy Rollers

Angular Accelerationt= I a t = fR

Linear AccelerationFtot = maFtot = mg sinq – f

a = a/R

ImR

gmRa

gmRaImR

mgR

Iama

R

Iamgma

R

Iaf

R

IaIfR

fmgma

2

2

22

2

2

2

sin

sin

sin

sin

sin

As I increases, a decreases

Page 21: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 21 of 31

Moment of Inertia

Let’s use conservation of energy

ghv

ghv

ImR

ghmRv

R

vImvImvmgh

disk

hoop

2817.

2707.

2

2

1

2

1

2

1

2

1

2

22

2

2222

Page 22: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 22 of 31

Moment of Inertia

• Which will have the greater acceleration?

• Which will have the greater angular acceleration?

m1 = 1 kg

F = 5 N

m2 = 2 kg

F = 5 N

F = 5 N

m = 1 kgr1 = 1 m r2 = 2 m

F = 5 N

m = 1 kg

F = maFr = mrat= mr2at = I aI = mR2

Page 23: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 23 of 31

Moment of Inertia

• What’s the moment of inertia of an extended object?

dmrrmrmrmrmIIII ii222

332

222

11321

2

2

1MRI 2

12

1MLI 2

3

1MLI

Page 24: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 24 of 31

Page 25: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 25 of 31

Moment of Inertia

Page 26: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 26 of 31

Conservation of Angular Momentum

Demo: Rotation with Weights

Conservation of L:L = Iw

If moment of inertia goes own, then angular velocity must go up.

Page 27: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 27 of 31

Conservation of Angular Momentum

Demo: Gyroscope

Demo: Gyro in a can

Demo: Wheel on a string

Page 28: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 28 of 31

Conservation of Angular Momentum

The total angular momentum vector must be conserved. If you flip the spinning wheel, then something else must create an angular momentum vector.

DEMO: Spinning Wheel and rotation chair

Page 29: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 29 of 31

Center of Gravity

The center of gravity (or Center of mass) is the point about which an object will rotate. For a body under goes both linear projectile motion and rotational motion, the location of the center of mass will behave as a free projectile, while the extended body rotates around the c.o.m.

Parabolic trajectory of the center of mass

Extended body rotating with constant angular velocity

Page 30: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 30 of 31

Center of Gravity

Angular impulse

Parabolic trajectory of the center of mass

Page 31: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 31 of 31

For point particle

Summary of Angular Equations

r

v

t

PrL

IL

Fr

t

LObject on Net

Direction of ω

Magnitude of ω

Same direction as Δω

For extended body

Point particle or extended body

Same direction as ΔL

2

2

1 IKErot For extended body

Page 32: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 32 of 31

Announcements

Page 33: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 33 of 31

DL Sections

Page 34: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 34 of 31

Conservation of Angular Momentum

Page 35: Physics 7B Lecture 824-Feb-2010 Slide 1 of 31 Physics 7B-1 (A/B) Professor Cebra Rotational Kinematics and Angular Momentum Conservation Winter 2010 Lecture

Physics 7B Lecture 824-Feb-2010 Slide 35 of 31

Torque