Newton’s Third Law of Motion
Claimed by Arohi Bhakhri
Forces are products of interactions between bodies and can be defined as a interaction that has some type of effect on the motion of an object when unopposed. Forces can result by a number of contact interactions (frictional, normal, tension, applied) or just interactions between some radius (gravitational, electrical, magnetic forces). Newton's Third Law of Motion states that when there is an interaction between two objects, they are both exerting forces upon each other. A simple example would be if you were sitting down on a bench--your body exerts the same amount of force on the bench that the bench exerts on your body, just in an opposite direction. These two forces are examples of action-reaction pairs, which is what Newton's Third Law is entirely based around. Formally stated, Newton's third law is: For every action, there is an equal and opposite reaction.
The Main Idea
As stated above, Newton's Third Law states that if object A exerts a force on object B, then object B also exerts an equal and opposite force on object A.
The third law means that all forces are interactions between different bodies, and thus that there is no such thing as a unidirectional force or a force that acts on only one body. This law is sometimes referred to as the action-reaction law, with FA called the "action" and FB the "reaction". The action and the reaction are simultaneous, and it does not matter which is called the action and which is called reaction; both forces are part of a single interaction, and neither force exists without the other.
A Mathematical Model
Using the system of A and B, we can say that the force of A on B is equal and opposite to that of B on A.
F(AB) = −F(BA)
A Computational Model
How do we visualize or predict using this topic. Consider embedding some vpython code here Teach hands-on with GlowScript
Examples
Elementary Example
If an astronaut is simply floating in deep space with only his space suit, is there any way for him to escape?
Solution: For two reasons, he is not able to escape. There is no matter in space which does not give the astronaut anything to exert a force upon to propel him in the desired direction. In addition, by Newton's Third Law, exerting a force on his own body would merely cause an action-reaction pair of forces that are equal an opposite and therefore exactly cancel out with each other--thus he is not able to move.
Intermediate Example
An 85 kg person is standing inside of an elevator that is accelerating at downwards at 0.45 m/s^2. Calculate the force the person exerts on the floor of the elevator.
We see Newton's Third Law in this example in that there is a action and reaction pair force between the floor and the person. The reaction force points upwards, opposite the direction of the force of the 85 kg person's weight. We can then invoke Newton's Second Law [1].
F = ma W - R = ma = 85 kg x 0.45 m/s^2 R = W - 85 kg x 0.45 m/s^2 R = 85 kg × 9.81 m/s^2 − 85 kg × 0.45 m/s^2 = 795.6 N
Advanced Example
One implication of Newton's Third Law is the Law of Conservation of Momentum. Two carts, cart 1 and cart 2, collide with one another on a track. How does the momentum of each cart change as they collide and after the collision, what happens to the momentum of the two-cart system? The upward normal force applied by the track on each cart is balanced by the downward force of gravity, so the net force experienced by each cart during the collision is that applied by the other cart.
The collision changes the momentum of cart 1 from
p1i to p1f = p1i + deltap1.
Similarly, the collision changes the momentum of cart 2 from
p2i to p2f = p2i + deltap2.
The total momentum of the system beforehand is
p1i + p2i.
The total momentum of the system afterwards is
p1f + p2f = p1i + deltap1 + p2i + deltap2.
Consider deltap1--This change in momentum comes from the force applied to cart 1 by cart 2 during the collision. Similarly, deltap2 comes from the force applied to cart 2 by cart 1 during the collision. Newton’s third law tells us that, no matter what, the force applied to cart 1 by cart 2 is equal and opposite to that applied to cart 2 by cart 1.
deltap2 = -deltap1 (Doesn't this look similar to something we already know?)
Substituting this result into our expression for the total momentum of the system after the collision shows that momentum is conserved (momentum remains constant):
p1f + p2f = p1i + p2i
Connectedness
How is this topic connected to something that you are interested in? Newton's Third Law is integral to understanding motion and why it occurs a certain way. Having played soccer for several years, understanding why this law works the way it does helps in performance during matches. From Newton’s first law, it is known that the soccer ball’s motion could not have changed unless a force acted on it--i.e. an interaction is required to produce a force. Every time a soccer ball is kicked, this law comes into play. A force from the foot is exerted onto the ball--this force is called an action force. At the same time, the ball exerts a force on your foot as it is in contact with the ball. This force is called a reaction force. Humans can be considered to be more massive to the ball so it is hard to realize that the soccer ball does produce a reaction force against the foot kicking it.
How is it connected to your major? Industrial and systems engineering is a branch of engineering which deals with the optimization of complex processes or systems. Industrial engineers work to decrease or eliminate altogether the waste of time, money, materials, labor, operation times, energy and other resources that hinder the ability to generate value. According to the Institute of Industrial and Systems Engineers (IISE), at the basic level, their job is to figure out how to do better. They engineer processes and systems that improve quality and productivity in all branches of production and business. Having noted this, there is a physics behind productivity, especially in manufacturing firms where any extra force or motion of a machine can be holding back greater efficiency of production as a whole.
History
In 1686, Sir Issac Newton presented his three laws of motion in the "Principia Mathematica Philosophiae Naturalis." Newton's three laws of motion are integral to understanding why forces have the effect they do upon other bodies. In the English translation of the third edition of the Principia Newton's own statement of the third law of motion reads exactly "To every action there is always opposed an equal reaction; or the mutual actions of the two bodies upon each other are always equal, and directed to contrary parts". Newton's examples, immediately following this statement, include the forces of a finger on a stone and the stone on the finger, the forces between a horse and a stone (both of which are connected by a rope), the forces between two colliding bodies, and 'attractions' between objects - that is, forces, such as gravity, which act at a distance rather than through direct contact
See also
The following links are for furthering understanding of Newton's Third Law and also practice examples.
Additional reading
Read Newton's Principia Here --> [2]
The Physics Classroom on Newton's Third Law --> [3]
External links
Watch the Best Film on Newton's Third Law. Ever. (video) --> [4]
Experiment with Newton's Third Law with these easy demos --> [5]
Newton's Third Law is just rocket science (video) --> [6]