torque

25
Torque We know that Newton’s second law ( ) explains that the net force is the source of an object’s acceleration. What is the source of a rotating object’s angular acceleration? It can’t be just a force, because it matters where on the object that force is applied. The answer lies in the quantity called torque. F ma

Upload: tara-rollins

Post on 30-Dec-2015

16 views

Category:

Documents


0 download

DESCRIPTION

Torque. We know that Newton’s second law ( ) explains that the net force is the source of an object’s acceleration. What is the source of a rotating object’s angular acceleration? It can’t be just a force, because it matters where on the object that force is applied. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Torque

Torque

We know that Newton’s second law ( ) explains that the net force is the source of an object’s acceleration.

What is the source of a rotating object’s angular acceleration? It can’t be just a force, because it matters where on the object that force is applied.

The answer lies in the quantity called torque.

F ma

Page 2: Torque

Torque…

Torque, , is the tendency of a force to rotate an object about some axis Torque is a vector = r F sin = F d

F is the force is the angle the force makes with the horizontal d is the moment arm (or lever arm)

Page 3: Torque

…Torque…

The moment arm, d, is the perpendicular distance from the axis of rotation to a line drawn along the direction of the force d = r sin Φ

Page 4: Torque

…Torque

The horizontal component of F (F cos ) has no tendency to produce a rotation

Torque will have direction If the turning tendency of the force is

counterclockwise, the torque will be positive If the turning tendency is clockwise, the torque will

be negative

Page 5: Torque

You are trying to open a door that is stuck by pulling on the doorknob in a direction perpendicular to the door. If you instead tie a rope to the doorknob and then pull with the same force, is the torque you exert increased?

A.yes

B.no

Conceptest…

Page 6: Torque

You are trying to open a door that is stuck by pulling on the doorknob in a direction perpendicular to the door. If you instead tie a rope to the doorknob and then pull with the same force, is the torque you exert increased?

A.yes

B.no

…Conceptest

Page 7: Torque

You are using a wrench and trying to loosen a rusty nut. Which of the arrangements shown is most effective in loosening the nut? List in order of descending efficiency the following arrangements:

                                                                 

Conceptest…

Page 8: Torque

You are using a wrench and trying to loosen a rusty nut. Which of the arrangements shown is most effective in loosening the nut? List in order of descending efficiency the following arrangements:

                                                                 

…Conceptest

Page 9: Torque

A plumber pushes straight down on the end of a long wrench as shown. What is the magnitude of the torque he applies about the pipe at lower right?

A. (0.80 m)(900 N)sin 19°

B. (0.80 m)(900 N)cos 19°

C. (0.80 m)(900 N)tan 19°

D. none of the above

Conceptest…

Page 10: Torque

A. (0.80 m)(900 N)sin 19°

B. (0.80 m)(900 N)cos 19°

C. (0.80 m)(900 N)tan 19°

D. none of the above

A plumber pushes straight down on the end of a long wrench as shown. What is the magnitude of the torque he applies about the pipe at lower right?

…Conceptest

Page 11: Torque

Net Torque

The force F1 will tend to cause a counterclockwise rotation about O

The force F2 will tend to cause a clockwise rotation about O

F1d1 – F2d2

Page 12: Torque

Torque vs. Force Forces can cause a change in linear

motion Described by Newton’s Second Law

Forces can cause a change in rotational motion The effectiveness of this change depends on

the force and the moment arm The change in rotational motion depends on

the torque

Page 13: Torque

Torque Units

The SI units of torque are N.m Although torque is a force multiplied by a

distance, it is very different from work and energy The units for torque are reported in N.m and not

changed to Joules

Page 14: Torque

Torque and Angular Acceleration, Wheel Example The wheel is rotating

and so we apply The tension supplies the

tangential force

The mass is moving in a straight line, so apply Newton’s Second Law Fy = may = mg - T

Page 15: Torque

Torque and Angular Acceleration, Multi-body Ex.,

1 Both masses move in linear directions, so apply Newton’s Second Law

Both pulleys rotate, so apply the torque equation

Page 16: Torque

Torque and Angular Acceleration, Multi-body Ex.,

2

The mg and n forces on each pulley act at the axis of rotation and so supply no torque

Apply the appropriate signs for clockwise and counterclockwise rotations in the torque equations

Page 17: Torque

Problem

A model airplane with mass 0.750 kg is tethered by a wire so that it flies in a circle 30.0 m in radius. The airplane engine provides a net thrust of 0.800 N perpendicular to the tethering wire.

(a) Find the torque the net thrust produces about the center of the circle.

(b) Find the angular acceleration of the airplane when it is in level flight.

(c) Find the linear acceleration of the airplane tangent to its flight path.

Page 18: Torque

Answers

a) 24.0 N-m

b) 0.0356 rad/s2

c) 1.07 m/s2

Page 19: Torque

Review: The Vector Product

Given two vectors, A and B

The vector (“cross”) product of A and B is defined as a third vector, C

C is read as “A cross B”

The magnitude of C is AB sin is the angle between A and B

Page 20: Torque

More About the Vector Product

The quantity AB sin is equal to the area of the parallelogram formed by A and B

The direction of C is perpendicular to the plane formed by A and B

The best way to determine this direction is to use the right-hand rule

Page 21: Torque

Properties of the Vector Product

The vector product is not commutative. The order in which the vectors are multiplied is important

To account for order, rememberA x B = - B x A

If A is parallel to B ( = 0o or 180o), then A x B = 0 Therefore A x A = 0

Page 22: Torque

Vector Products of Unit Vectorsˆ ˆ ˆ ˆ ˆ ˆ 0

ˆ ˆ ˆ ˆ ˆ

ˆ ˆ ˆˆ ˆ

ˆ ˆ ˆˆ ˆ

i i j j k k

i j j i k

j k k j i

k i i k j

Signs are interchangeable in cross productsA x (-B) = - A x B

ˆ ˆ ˆ ˆ i j i j

Page 23: Torque

The Vector Product and Torque

The torque vector lies in a direction perpendicular to the plane formed by the position vector and the force vector

= r x F

The torque is the vector (or cross) product of the position vector and the force vector

Page 24: Torque
Page 25: Torque

Torque Vector Example

Given the force

= ?

m)ˆ00.5ˆ00.4(

N)ˆ00.3ˆ00.2(

jir

jiF

ˆ ˆ ˆ ˆ [(4.00 5.00 )N] [(2.00 3.00 )m]

ˆ ˆ ˆ ˆ[(4.00)(2.00) (4.00)(3.00)

ˆ ˆ ˆ ˆ(5.00)(2.00) (5.00)(3.00)

ˆ2.0 N m

r F i j i j

i i i j

j i i j

k