Consider the following situations:

- You and a friend are sitting on chairs with rollers. You both have your feet off the ground and with your feet you push against your friend's chair. Your friend starts moving away from you and you start moving away from your friend. You both are accelerating. The direction of your acceleration is opposite to the direction of your friend's acceleration.
- You both stretch out your hands and you grab your friend and pull him towards you. He accelerates towards you and you accelerate towards him. Again you both are accelerating.

What is happening is a consequence of **Newton's third law**.

For every force that an
object exerts on a second object, there is a force equal in magnitude but
opposite in direction exerted by the second object on the first object.
Forces are the result of** interactions.**You pull on me, I pull on you. If no other forces are present, I will accelerate towards you. My acceleration has
the magnitude of the force divided by

You push against the table, the table pushes against you. You
accelerate away from the table. **Why is the table not accelerating away from you?
**Answer:

If the table is on rollers, it will accelerate away from you. If the table is very massive, the magnitude of its acceleration will be much smaller than the magnitude of your acceleration. If it is not on rollers, then the force of static friction is also acting on it, and the vector sum of the two forces is zero.

Standing on a very slippery surface or on a skateboard, you throw a heavy object away from you in a northerly direction. To do this, you have to exert a force on the object in the northerly direction. The object exerts a force on you, which has equal magnitude but points towards the south. You accelerate southward.

Newton's third law is also called the **law of
action and reaction**.
For every action force, there exists a reaction force, equal in magnitude and
opposite in direction.**
The action and reaction force always act on different objects. **
The objects interact.

Note: Two forces acting on the same object, even if they have the same magnitude and point in opposite direction, never form an action-reaction pair.

An apple with a 0.2 kg mass sits on a table in equilibrium.

(a) What forces act on it? Provide their magnitude and direction.

(b) What is the reaction force to each of the forces acting on the apple?

(c) What are the action-reaction pairs?

Solution:

(a) The forces acting on the apple are its weight W = mg = 1.96 N pointing
down and the normal force provided by the table F_{N} = 1.96 N
pointing up. The net force acting on the apple is zero.

(b) The reaction force to W is a force F_{WR} = 1.96 N pointing up acting
on the center of the Earth. (The earth is pulling on the apple and the
apple is pulling on the earth.)

The reaction to F_{N} is a force F_{NR} = 1.96 N pointing
down acting on the table. (The table is pushing up on the apple, the
apple is pushing down on the table.)

(c) The action-reaction pairs are W − F_{WR} and N − F_{NR}.

While a football is in flight, what forces act on it? What are the action and reaction pairs while the football is being kicked and while it is in flight?

Solution:

While in flight, gravity and air friction act on the ball.

When the ball is being kicked, the earth pulls on the ball downward
(gravity), the ball pulls on the earth upward (gravity). The foot pushes
the ball forward, the ball pushes the foot backward.

When the ball is in
flight, the earth pulls on the ball downward (gravity), the ball pulls on
the earth upward (gravity). The ball pushes the air forward and the air
pushes the ball backward.

Newton's second law: **F**_{net} = m**a**

To find the net force on an object, all the vector forces that act
on the object have to be added. We use **free-body diagrams** to help us with this task. Free-body
diagrams are diagrams used to show the relative magnitude and direction
of all forces acting on an object in a given situation. The object is
represented by a box or some other simple shape. The forces are represented by arrows. The length
of the arrow in a free-body diagram is proportional the magnitude of the
force. The direction of the arrow gives the direction of the force.
Each force arrow in the diagram is labeled. All forces, which act on
the object, must be represented in the free-body diagram. A free body
diagram only includes the forces that act on the object, not the forces
the object itself exerts on other objects.

A free-body diagram for a freely falling ball:

Neglecting air friction, the only force acting on the ball is gravity.

A free-body diagram for a ball resting on the ground:

Gravity is acting downward. The ball is at rest. The ground must exert
a force equal in magnitude and opposite in direction on the ball. This
force is called the **normal force, n**, since it is normal to the surface.

A free-body diagram for a mass on an inclined plane:

Gravity acts downward. The component of
**F**_{g}
perpendicular to the surface is cancelled out by the normal force the
surface exerts on the mass. The mass does not accelerate in the
direction perpendicular to the surface. The component of **F**_{g}
parallel to the surface causes the mass to accelerate in that direction.

Assume your team and an opposing team are pulling on a rope in opposite
directions. The rope starts accelerating in the direction of the
opposing team.

What is the net force on the rope?

Answer:

It is the vector sum of the force of gravity and the forces
exerted by the two teams.

Which team is exerting the greater force?

Answer:

The opposing team, since the rope starts accelerating in their
direction.

Is there a net force on the rope if the rope is not accelerating, even so each team is pulling as hard as it can?

Answer:

No, there is no net force. However, there is **tension** in the
rope. Tension results from different forces acting on different parts of
the body. Tension can break things. A pure force, i.e. the same force
acting on all parts of the body, cannot break things.

If instead of
pulling on the rope the two teams push on a heavy rock, but the rock does
not move, then again the net force on the rock is zero. However, now the
rock is under **compression**.

The tension T is a scalar. It is defined as the magnitude of the
force with which the stretched rope pulls on whatever it is attached to.
This force is often denoted by **T**. The direction of
**T**
depends on which end of the rope is being considered.

The net force acting on an object is always the vector sum of all forces acting on an object. The object's acceleration is in the direction of this net force and has magnitude a = (net force/object's mass).

A 15-lb block rests on the floor. (Note: lb is a
unit of force, the weight of the block is 15 lb.)

(a) What
force does the floor exert on the block?

(b) If a rope is tied to
the block and run vertically over a pulley and the other end is attached to
a free-hanging 10-lb weight, what is the force exerted by the floor on the
15-lb block?

(c) If we replace the 10-lb weight in part (b) with a
20-lb weight, what is the force exerted by the floor on the 15-lb block?

Solution:

(a) The block is at
rest the net force is zero. The weight of the block is 15 lb
downward. The floor must therefore exert a force 15 lb upward.

(b)
The block is still at rest.
The weight is 15 lb downward, the rope pulls with 10 lb upward
due to the tension in the rope. The floor must therefore
exert a force 5 lb upward.

(c) The weight is 15 lb downward,
the rope pulls with 20 lb upward due to the tension in the rope.
The block will accelerate upward, since the net force is upward.
The block is not pushing on the ground, and the ground is not
pushing back. The ground exerts zero force on the block.

(a) Find the tension in each of the cords of the system shown in the figure below. Neglect the masses of the cords.

(b) Find the tension in each of the cords of the system shown in the figure below. Neglect the masses of the cords.

Solution:

(a) The mass is not accelerating, it is in **equilibrium**. The net force on the mass is zero.

We therefore
have T_{3 }= mg = 49 N.

The
knot in the cable is in equilibrium. The net force on the knot is
zero. F_{x }= 0, F_{y }= 0.

∑F_{ix }= 0, ∑F_{iy
}= 0. Adding the x-components of all forces in the diagram we
obtain

F_{x }= -T_{1}cos40^{o }+ T_{2}cos50^{o
}= 0 , or T_{2 }= T_{1}cos40^{o}/cos50^{o
}= 0.192 T_{1}.

Adding the
y-components we obtain F_{y}= T_{1}sin40^{o }+ T_{2}sin50^{o
}- T_{3 }= 0,

or 0.643 T_{1 }+ 1.192 T_{1}*0.766
= 49 N, 1.556T_{1 }= 49 N, T_{1 }= 31.5 N, T_{2 }= 37.54 N.

(b) The mass is not accelerating, it is in equilibrium.
The net force on the mass is zero.

We therefore have T_{3
}= mg = 98 N.

The knot in the cable is in equilibrium. The
net force on the knot is zero. F_{x }= 0, F_{y }=
0.

∑F_{ix }= 0, ∑F_{iy }= 0. Adding the
x-components of all forces in the diagram we obtain

F_{x }=
-T_{1}cos60^{o }+ T_{2 }= 0, or T_{2 }=
T_{1}cos60^{o }= 0.5T_{1}.

Adding the
y-components we obtain F_{y }= T_{1}sin60^{o }-
T_{3 }= 0, or 0.866 T_{1 }= 98 N,

T_{1 }=
113.2 N, T_{2 }= 56.6 N.