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Physics 1.6 - Forces (moment and Center of mass)

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PHYSICS – Forces 2 Moments
LEARNING
OBJECTIVES
1.5.2 Turning effect
Core
• Describe the moment of a force as a
measure of its turning effect and give
everyday examples
• Understand that increasing force or
distance from the pivot increases the
moment of a force
• Calculate moment using the product
force × perpendicular distance from the
pivot
• Apply the principle of moments to the
balancing of a beam about a pivot
Supplement
• Apply the principle of moments to
different situations
1.5.3 Conditions for equilibrium
Core
• Recognise that, when there is no
resultant force and no resultant turning
effect, a system is in equilibrium
• Perform and describe an experiment
(involving vertical forces) to show that
there is no net moment on a body in
equilibrium
LEARNING
OBJECTIVES
1.5.2 Turning effect
Core
• Describe the moment of a force as a
measure of its turning effect and give
everyday examples
• Understand that increasing force or
distance from the pivot increases the
moment of a force
• Calculate moment using the product
force × perpendicular distance from the
pivot
• Apply the principle of moments to the
balancing of a beam about a pivot
Supplement
• Apply the principle of moments to
different situations
1.5.3 Conditions for equilibrium
Core
• Recognise that, when there is no
resultant force and no resultant turning
effect, a system is in equilibrium
• Perform and describe an experiment
(involving vertical forces) to show that
there is no net moment on a body in
equilibrium
Forces and moments
Spanners are
used for
tightening and
loosening nuts.
They help to
produce a
larger turning
effect.
Forces and moments
Spanners are
used for
tightening and
loosening nuts.
They help to
produce a
larger turning
effect.
The longer
the spanner,
the greater
the turning
effect (force)
Forces and moments
Spanners are
used for
tightening and
loosening nuts.
They help to
produce a
larger turning
effect.
The longer
the spanner,
the greater
the turning
effect (force)
Forces and moments
Moment of = force x perpendicular
a force about
distance from
a point
the point
Forces and moments
Moment of = force x perpendicular
a force about
distance from
a point
the point
Moments may be described as clockwise or
anticlockwise, and the moment of a force is
also called a torque.
Forces and moments
Don’t
forget
that the
unit of
Force ie
the
Newton
(N)
Moment of = force x perpendicular
a force about
distance from
a point
the point
Moments may be described as clockwise or
anticlockwise, and the moment of a force is
also called a torque.
Forces and moments
To increase the force
applied to undoing a
wheel nut, extend the
length of the spanner –
you can do this by
inserting a length of
pipe over the end.
Let’s look at a
few examples
of calculations
involving
moments.
4m
X
5N
Moment about X = 5 x 4 = 20N
(clockwise)
3N
Let’s look at a
few examples
of calculations
involving
moments.
X
5m
Moment about X = 3 x 5 = 15N
(anticlockwise)
4m
X
5N
Moment about X = 5 x 4 = 20N
(clockwise)
3N
Let’s look at a
few examples
of calculations
involving
moments.
X
5m
Moment about X = 3 x 5 = 15N
(anticlockwise)
4m
X
5N
Moment about X = 5 x 4 = 20N
(clockwise)
Principle of moments
LEARNING
OBJECTIVES
1.5.2 Turning effect
Core
• Describe the moment of a force as a
measure of its turning effect and give
everyday examples
• Understand that increasing force or
distance from the pivot increases the
moment of a force
• Calculate moment using the product
force × perpendicular distance from the
pivot
• Apply the principle of moments to the
balancing of a beam about a pivot
Supplement
• Apply the principle of moments to
different situations
1.5.3 Conditions for equilibrium
Core
• Recognise that, when there is no
resultant force and no resultant turning
effect, a system is in equilibrium
• Perform and describe an experiment
(involving vertical forces) to show that
there is no net moment on a body in
equilibrium
The Principle of Moments
This beam is in a state of
balance.
The Principle of Moments
This beam is in a state of balance.
In order to be balanced, the clockwise forces
must be equal to the anticlockwise forces.
We say that the beam is in a state of
equilibrium.
The Principle of Moments
The Principle of Moments states that:
“If an object is in equilibrium, the sum of the
clockwise moments about any point is equal to the
sum of the anticlockwise moments about that
point.”
The Principle of Moments
1m
Let’s look
at some
worked
examples
2m
X
20N
Anticlockwise moment
= 20 x 1 = 20Nm
10N
Clockwise moment
= 10 x 2 = 20Nm
The Principle of Moments
1m
Let’s look
at some
worked
examples
2m
0.5m
X
20N
Anticlockwise moment
= 20 x 1 = 20Nm
20N
5N
Combined clockwise moment
= (5 x 2) + (20 x 0.5) = 20Nm
The Principle of Moments
Hitching point
What force does the
trailer exert on the
hitching point, and
what force do the
rear tyres exert on
the road?
Rear tyres
(consider as a
single force)
The Principle of Moments
Centre of
mass of
trailer
6m
3m
400 kN
What force does the
trailer exert on the
hitching point, and
what force do the rear
tyres exert on the
road?
The Principle of Moments
Centre of
mass of
trailer
X
6m
3m
A
At the hitching point,
the downward force of
the trailer on the hitch
is equal to the upward
force of the hitch on
the trailer (X).
400 kN
What force does the
trailer exert on the
hitching point, and
what force do the
rear tyres exert on
the road?
The Principle of Moments
Centre of
mass of
trailer
X
At the hitching point,
the downward force of
the trailer on the hitch
is equal to the upward
force of the hitch on
the trailer (X).
Y
6m
3m
A
What force does the
trailer exert on the
hitching point, and
what force do the
rear tyres exert on
the road?
400 kN
B
The downward force of
the rear tyres on the
road is equal to the
upward force of the road
on the tyres (Y).
The Principle of Moments
Centre of
mass of
trailer
X
Y
6m
3m
A
What force does the
trailer exert on the
hitching point, and
what force do the
rear tyres exert on
the road?
400 kN
To find X, look at the moments about point B
Clockwise moment = X x 9m
Anticlockwise moment = 400kN x 6m = 2400kN m
X x 9m = 2400 kN m
So: X = 266.7 kN
So: downward force on hitching point = 266.7kN
B
The Principle of Moments
Centre of
mass of
trailer
X
Y
6m
3m
A
What force does the
trailer exert on the
hitching point, and what
force do the rear tyres
exert on the road?
400 kN
B
To find Y:
Total upward force = Total downward force
So:
X + Y = 400kN
So: 266.7 + Y = 400kN
So:
Y = 400kN - 266.7kN
Y = 133.3kN
So: the downward force from rear tyres = 133.3kN
LEARNING
OBJECTIVES
1.5.2 Turning effect
Core
• Describe the moment of a force as a
measure of its turning effect and give
everyday examples
• Understand that increasing force or
distance from the pivot increases the
moment of a force
• Calculate moment using the product
force × perpendicular distance from the
pivot
• Apply the principle of moments to the
balancing of a beam about a pivot
Supplement
• Apply the principle of moments to
different situations
1.5.3 Conditions for equilibrium
Core
• Recognise that, when there is no
resultant force and no resultant turning
effect, a system is in equilibrium
• Perform and describe an experiment
(involving vertical forces) to show that
there is no net moment on a body in
equilibrium
PHYSICS – Forces 3. Centre of mass.
LEARNING
OBJECTIVES
1.5.4 Centre of mass
Core
• Perform and describe an experiment
to determine the position of the centre
of mass of a plane lamina
• Describe qualitatively the effect of
the position of the centre of mass on
the stability of simple objects
1.5.5 Scalars and vectors
Supplement
• Understand that vectors have a
magnitude and direction
• Demonstrate an understanding of the
difference between scalars and vectors
and give common examples
• Determine graphically the resultant of
two vectors
Centre of Mass
Upward
force on
ruler
Centre of Mass
Upward force
on ruler
Suspension
point (G)
Lots of tiny particles
exerting gravitational forces
on either side of point G
When the gravitational
forces on either side of G
are equal, the ruler is
balanced.
The forces now act together at G
(a resultant force) = the weight.
G is the centre of mass, or
centre of gravity.
LEARNING
OBJECTIVES
1.5.4 Centre of mass
Core
• Perform and describe an experiment
to determine the position of the centre
of mass of a plane lamina
• Describe qualitatively the effect of
the position of the centre of mass on
the stability of simple objects
1.5.5 Scalars and vectors
Supplement
• Understand that vectors have a
magnitude and direction
• Demonstrate an understanding of the
difference between scalars and vectors
and give common examples
• Determine graphically the resultant of
two vectors
So how do you find the
centre of mass (centre of
gravity) for an irregularly
shaped object?
So how do you find the
centre of mass (centre of
gravity) for an irregularly
shaped object?
Allow the card to
swing freely from
the pin.
So how do you find the
centre of mass (centre of
gravity) for an irregularly
shaped object?
Allow the card to
swing freely from
the pin.
The card turns
until the centre of
mass is vertically
under the pin.
So how do you find
the centre of mass
(centre of gravity) for
an irregularly shaped
object?
Allow the card to
swing freely from
the pin.
The card turns
until the centre of
mass is vertically
under the pin.
Repeat using a
plumb line, and
wherever the
lines cross, this
is the centre of
mass.
LEARNING
OBJECTIVES
1.5.4 Centre of mass
Core
• Perform and describe an experiment
to determine the position of the centre
of mass of a plane lamina
• Describe qualitatively the effect of
the position of the centre of mass on
the stability of simple objects
1.5.5 Scalars and vectors
Supplement
• Understand that vectors have a
magnitude and direction
• Demonstrate an understanding of the
difference between scalars and vectors
and give common examples
• Determine graphically the resultant of
two vectors
Centre of Mass and Stability
If a force is applied, which box
will be the most stable?
Centre of Mass and Stability
Centre of mass
Weight acting downwards
Upward force from ground
The box here is in equilibrium. Forces are
balanced, as are the turning effects.
Centre of Mass and Stability
If a small force is applied, the tilt is small and
the upward and downward forces will act to
return the box to its original position.
Centre of Mass and Stability
With a larger force applied there is more tilt,
the box goes beyond the centre of gravity, so
will fall over.
Centre of Mass and Stability
If the box has a wider base and a lower
centre of gravity then it will be harder to tip
over.
Centre of Mass and Stability
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