Torque & Rotational Inertia Lecturer: Professor Stephen T. Thornton

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Torque & Rotational Inertia Lecturer: Professor Stephen T. Thornton

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Torque & Rotational Inertia Lecturer: Professor Stephen T. Thornton. Reading Quiz. A) F 1 B) F 3 C) F 4 D) all of them E) none of them. - PowerPoint PPT Presentation

Transcript of Torque & Rotational Inertia Lecturer: Professor Stephen T. Thornton

Page 1: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Torque & Rotational Inertia

Lecturer: Professor Stephen T. Thornton

Page 2: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Reading QuizReading QuizIn which of the cases shown below

is the torque provided by the

applied force about the rotation

axis biggest? For all cases the

magnitude of the applied force is

the same.

A) F1

B) F3

C) F4

D) all of them

E) none of them

Page 3: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Reading QuizReading Quiz

A) F1

B) F3

C) F4

D) all of them

E) none of them

In which of the cases shown below

is the torque provided by the

applied force about the rotation

axis biggest? For all cases the

magnitude of the applied force is

the same.

The torque is == F d sin F d sin

and so the force that is at 90°90°

to the lever arm is the one that

will have the largest torquelargest torque.

Clearly, to close the door, you

want to push perpendicularlyperpendicularly!!

Page 4: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Last TimeBegan angular motion

Angular position, displacement

Angular speed, velocity

Angular acceleration

Similarities between translation and rotation

Page 5: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Today

Torque

Rotational inertia (moment of inertia)

Rotational kinetic energy

Page 6: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

What is torque?

We recognize there is a relationship between tangential force and making something rotate.

first, simple definitionrF

Page 7: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Only the Tangential Component of a Force Causes a Torque

is angle between and r F

Page 8: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

The Moment Arm

sin

r

F

F

F

r

r

moment arm

Page 9: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Sign convention for torque according to most textbooks:

> 0 if the torque causes a CCW acceleration.

< 0 if the torque causes a CW acceleration.

Page 10: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz:You are using a wrench to loosen a rusty nut. Which of the arrangements below is least effective in loosening the nut? Force is proportional to length of vector.

A.

B.

C.

D.

E. not possible to determine

A

C

B

D

Page 11: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Answer: C

The force vectors are all the same. The arrangement that is the least effective is the one with the shortest moment arm. That is C.

Page 12: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz:A mechanic is finding it very difficult to muster enough torque to twist a stubborn bolt with a wrench, and she wishes she had a length of pipe to place over the wrench handle to increase her leverage. Will torque be increased if the mechanic pulls just as hard on a length of rope tied to the wrench handle?

 

A) Yes B) No C) Only in space. D) Not enough information given.

Page 13: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Answer: B (no)The rope placed in this position neither increases the force or the moment arm (length of application of the force causing the torque).

Page 14: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Angular Quantities

If the angular velocity of a rotating object changes, it has a tangential acceleration:

Even if the angular velocity is constant, each point on the object has a centripetal acceleration:

tana Ra=2

cp Ra a Rw= =

tan

dv da R R

dt dt

wa= = =

( )222

R

Rva R

R R

ww= = =

Page 15: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Torque and Angular Acceleration

Page 16: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Torque and angular acceleration

22

/ Newton's 2nd law

(last time )

multiply by ( / )

where and is

called the rotational inertia (or moment of inertia)

Newton's 2nd law for rotatio

t

a F m

a Fa r

r mrr r

r F rFI mr I

r mr mr I

I

n

Page 17: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Linear and angular quantities

Linear Angular

m I

a F

Page 18: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Similarities between linear and angular motion quantities ***

x

v

a

0 0

0 0 0 0

2 20 0 0 0

2 2 2 20 0 0 0

1 1( ) ( )

2 21 1

2 2

2 ( ) 2 ( )

v v at t

x x v v t t

x x v t at t t

v v a x x

Page 19: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Look at system of particles2

2 2 2 21 1 2 2 3 3

for a fixed axis

if ...

then for a fixed axis

i i ii i

i ii

m r

I m r m r m r m r

I

Page 20: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Kinetic Energy of a Rotating Object

massless rod

2 2

2 2

2

1 1( )

2 21

2

1 is the

2

rotational energy

K mv m r

K mr

K I

I is called rotational inertia

Page 21: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Kinetic Energy of a Rotating Object of Arbitrary Shape

21

2 i ii

K m v

Page 22: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Rotational InertiaMoment of Inertia

Rotational kinetic energy2 2 2

2 2

2

1 1

2 2

1

2

where

212

i i i ii i

i ii

i ii

K m v m r

K m r

I m r

I K

I appears to be quite useful!!

Page 23: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

The Rotational Inertia (Moment of Inertia) of a Hoop

M

2I MR

Page 24: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

The Rotational Inertia (Moment of Inertia) of a Disk

21

2I MR

This is almost certainly an example in textbook.

Use calculus to find this value.

2I R dm=ò

Page 25: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Rotational Dynamics; Torque and Rotational Inertia

The quantity is called the rotational

inertia of an object.

The distribution of mass matters here—these two objects have the same mass, but the one on the left has a greater rotational inertia, as so much of its mass is far from the axis of rotation.

2i iI m R

Page 26: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Rotational Inertia for Uniform, Rigid Objects of Various Shapes and Total Mass M

Do not memorize!!

Page 27: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Rotational Inertia for Uniform, Rigid Objects of Various Shapes and Total Mass M

Page 28: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Demos:Rotational inertia rodsMoment of Inertia wheel

2

2

1

2

where i i

K I

I m r

Page 29: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

If a physical object is available, the rotational inertia (moment of inertia) can be measured experimentally.

Otherwise, if the object can be considered to be a continuous distribution of mass, the rotational inertia may be calculated:

2I R dm=ò

Page 30: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

The parallel-axis theorem gives the rotational inertia about any axis parallel to an axis that goes through the center of mass of an object:

2CMI I Mh= +

ICMI

Page 31: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Falling Rod. A thin rod of length stands vertically on a table. The rod begins to fall, but its lower end does not slide. (a) Determine the angular velocity of the rod as a function of the angle it makes with the tabletop. (b) What is the speed of the tip of the rod just before it strikes the table?

Page 32: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz:A figure skater spins around with her arms extended. When she pulls in her arms, her rotational inertia 

A) increases. 

B) decreases. 

C) stays the same.

Page 33: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Answer: B, decreases

The mass stays the same, but the radius decreases for the mass in her arms. The I must decrease.

Page 34: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz A) A) solid

aluminum

B) hollow goldB) hollow gold

C) sameC) same

same mass & radius

solid hollow

Two spheres have the same radius and equal masses. One is made of solid aluminum, and the other is made from a hollow shell of gold. Which one has the bigger rotational inertia about an axis through its center?

Page 35: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz

same mass & radius

solid hollow

Two spheres have the same radius and equal masses. One is made of solid aluminum, and the other is made from a hollow shell of gold. Which one has the bigger rotational inertia about an axis through its center?

Rotational inertia depends on mass and distance from axis squared. It is bigger for the shell because its mass is located farther from the center.

A) A) solid aluminum

B) hollow goldB) hollow gold

C) sameC) same

Page 36: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Conceptual Quiz:Two wheels with fixed hubs, each having a mass of 1 kg, start from rest, and forces are applied as shown. Assume the hubs and spokes are massless, so that the rotational inertia is I = mR2. In order to impart identical angular accelerations, how large must F2 be?

A) 0.25 N B) 0.5 N C) 1.0 N D) 2.0 N E) 4.0 N

2

Fr

I mr

Page 37: Torque & Rotational Inertia  Lecturer:  Professor Stephen T. Thornton

Answer: D

The hint on the figure should help. You want Fr/I to be the same ratio. Fr/mr2 = F/mr, so F/r must have the same ratio = 2.