Understanding Torque: Definition, Sign, and Calculation, Study notes of Physics

An introduction to the concept of torque, a vector quantity derived from forces that causes rotational motion. The definition of torque, its relationship to force and moment arm, and how to determine the sign of torque. It also explains the vector product or cross product of vectors r and f to calculate torque. Taken from physics 3a: torque & equilibrium by shoup.

Typology: Study notes

Pre 2010

Uploaded on 09/17/2009

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Physics 3A: Torque & Equilibrium
Shoup โ€“ 111
Lets talk about what causes rotational motion
We know forces cause translational motion
Another vector quantity derived from forces cause
rotational motion.
This is Torque
Consider the figure below:
We define the torque as:
We can understand this by
considering how one opens
a door
You push perpendicular to
the door, the door rotates
You push parallel to the
door, the door does not
rotate
๎˜€
๎˜
r F sin
๎˜‚
(10.18)
Pushing parallel is the F cos ฯ† part => doesn't produce rotation
Pushing perpendicular is the F sin ฯ† part:
Another way to look at it is:
where r sin ฯ† is called the
moment arm of the force
Its the perpendicular distance
from the rotation axis to the line
of action
The larger the moment arm, the larger the torque
We also define the "sign" of the torque by "+" if its resulting
rotation would be counterclockwise, and by "-" if its resulting
rotation would be clockwise.
๎˜ƒ
๎˜„
F
๎˜…
rsin
๎˜†
๎˜‡
๎˜ƒ
๎˜„
r
๎˜…
Fsin
๎˜†
๎˜‡
Physics 3A: Torque & Equilibrium
Shoup โ€“ 112
๎˜ˆ๎˜Š๎˜‰
๎˜ˆ๎˜Œ๎˜‹
๎˜๎˜Ž๎˜‰
๎˜๎˜Ž๎˜‹
๎˜
Consider the figure to the right:
What is the sum or the net torque?
WARNING: torque is NOT a force.
force cause torque
torque depend on the force, but also on the point of
application of the force.
Torque is a vector quantity, so we need to define its direction
Consider when I push on the bicycle wheel.
When wheel is rotating counterclockwise, we said its angular
velocity is up (right-hand rule)
Seems natural to say a torque which produces counterclockwise
rotation should also be "up"
๎˜
net
๎˜‘
๎˜
1
๎˜’
๎˜
2
๎˜‘
F
1
d
1
๎˜“
F
2
d
2
Physics 3A: Torque & Equilibrium
Shoup โ€“ 113
If we choose this then we can define the torque mathematically as:
This is the "vector product" or
"cross product" of the vectors r
and F
The vector product of two vectors
is a vector, thus has a magnitude
and a direction
Magnitude of:
is:
The direction is given by the "right hand rule":
point fingers of right hand in direction of A (first vector)
curl fingers into B (second vector)
Thumb points in direction of C
๎˜”๎˜–๎˜•
๎˜—
๎˜˜
r
๎˜™
๎˜”
F
(10.10)
๎˜š
C
๎˜›
๎˜œ
A
๎˜
๎˜ž
B
C
๎˜Ÿ
!
C
๎˜
"
A
"
"
B
"
sin
#
(10.21)
Physics 3A: Torque & Equilibrium
Shoup โ€“ 114
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Physics 3A: Torque & Equilibrium

Shoup โ€“ 111

Lets talk about what causes rotational motion

We know forces cause translational motion Another vector quantity derived from forces causerotational motion. This is

Torque Consider the figure below: We define the torque as: We can understand this byconsidering how one opensa door You push perpendicular tothe door, the door rotates You push parallel to thedoor, the door does notrotate

r F sin

Pushing parallel is the

F cos

ฯ†^

part => doesn't produce rotation

Pushing perpendicular is the F sin

ฯ†^

part:

Another way to look at it is:

where r sin

ฯ†

is called the

moment arm of the force^ Its the perpendicular distancefrom the rotation axis to the lineof action^ The larger the moment arm, the larger the torque We also define the "sign" of the torque by "+" if its resulting

rotation would be counterclockwise, and by "-" if its resultingrotation would be clockwise.

F

 r^ sin

 r

F^ sin

Physics 3A: Torque & Equilibrium

Shoup โ€“ 112

Consider the figure to the right:

What is the sum or the net torque? WARNING

: torque is

NOT

a force.

force cause torque torque depend on the force, but also on the point ofapplication of the force. Torque is a vector quantity, so we need to define its direction

Consider when I push on the bicycle wheel. When wheel is rotating counterclockwise, we said its angularvelocity is up (

right-hand rule

Seems natural to say a torque which produces counterclockwiserotation should also be "up"

 net

 F 1

d 1

 F 2

d 2

Physics 3A: Torque & Equilibrium

Shoup โ€“ 113

If we choose this then we can define the torque mathematically as:

This is the "

vector product

" or

" cross product

" of the vectors

r

and

F

The vector product of two vectorsis a vector, thus has a magnitudeand a direction Magnitude of:is: The direction is given by the "right hand rule":^ point fingers of right hand in direction of A (first vector)^ curl fingers into B (second vector)^ Thumb points in direction of C

r

  F^

 C

A

B

C

!  C

" A

"" B^ sin

Physics 3A: Torque & Equilibrium

Shoup โ€“ 114

Example: Properties:

ฮธ^ is angle between vectors if^

ฮธ^ = 0, cross-product is zero. if^

ฮธ^ = 180, cross-product is zero. (i.e.

if vectors are parallel, then cross-product is zero

Order of cross-product matters

For unit vectors:

i

i

j

j

k

j

0

i

j

k^ ^ j

k

i

 k

i

j

Physics 3A: Torque & Equilibrium

Shoup โ€“ 115

A^

B

B^

A

Now we can apply the concepts of torque and force to rigid bodies

Consider 1

st^ rigid bodies in "

equilibrium

This means the net force on the body is zero, and the nettorque on the body is zero:^ note:

these are the sum of all

external

forces and torque

In the general case 10.24 & 10.25 represent six scalarequations We will limit ourselves to "co-planar" forces, so that we onlyhave 3 equations:

^0

Physics 3A: Torque & Equilibrium

Shoup โ€“ 116

^ F^

^ F^ x

F^ y^

z^

Problem solving guidelines:

As always, draw a diagram of body Draw a free-body diagram of object, locating all forces beingapplied and what you think their directions are. Choose a coordinate system, aligned with one or more forces Resolve forces into x & y components and apply equilibriumforce equations Choose axis of rotation and compute torques do to all appliedforces^ Don't choose axis through application point of force you needto find.^ Do choose axis through forces which you don't care about. Apply equilibrium torque equation. Solve set of simultaneous equations for what you need. Do Example:

(Ch 10, #27, p. 354)

Physics 3A: Torque & Equilibrium

Shoup โ€“ 117