4.4 Newton’s Third Law

We have thus far considered force as a push or a pull; however, if you think about it, you realize that no push or pull ever occurs by itself. When you push on a wall, the wall pushes back on you. This brings us to Newton’s third law.

Baseball relief pitcher Mariano Rivera was so highly regarded that during his retirement year, opposing teams conducted farewell presentations when he played at their stadiums. The Minnesota Twins offered a unique gift: A chair made of broken bats. Any pitch can break a bat, but with Rivera’s signature pitch—known as a cutter—the ball and the bat frequently came together at a point that shattered the hardwood. Typically, we think of a baseball or softball hitter exerting a force on the incoming ball, and baseball analysts now focus on the resulting “exit velocity” as a key statistic. But the force of the ball can do its own damage. This is exactly what happens whenever one body exerts a force on another—the first also experiences a force (equal in magnitude and opposite in direction). Numerous common experiences, such as stubbing a toe or pushing off the floor during a jump, confirm this. It is precisely stated in Newton’s third law of motion.

We can readily see Newton’s third law at work by taking a look at how people move about. Consider a swimmer pushing off the side of a pool (Figure 4.16). She pushes against the wall of the pool with her feet and accelerates in the direction opposite that of her push. The wall has exerted an equal and opposite force on the swimmer. You might think that two equal and opposite forces would cancel, but they do not because they act on different systems. In this case, there are two systems that we could investigate: the swimmer and the wall. If we select the swimmer to be the system of interest, as in the figure, then [latex]{F}_{\text{wall on feet}}[/latex] is an external force on this system and affects its motion. The swimmer moves in the direction of this force. In contrast, the force [latex]{F}_{\text{feet on wall}}[/latex] acts on the wall, not on our system of interest. Thus, [latex]{F}_{\text{feet on wall}}[/latex] does not directly affect the motion of the system and does not cancel [latex]{F}_{\text{wall on feet}}.[/latex] The swimmer pushes in the direction opposite that in which she wishes to move. The reaction to her push is thus in the desired direction. In a free-body diagram, such as the one shown in Figure 4.16, we never include both forces of an action-reaction pair; in this case, we only use [latex]{F}_{\text{wall on feet}}[/latex], not [latex]{F}_{\text{feet on wall}}[/latex].

Other examples of Newton’s third law are easy to find:

• As a professor paces in front of a whiteboard, he exerts a force backward on the floor. The floor exerts a reaction force forward on the professor that causes him to accelerate forward. This is one of the most common examples of a reaction force in biomechanics. This reaction force exerted by the ground is essential to all forms of locomotion and is frequently investigated in the context of gait, jumping, and so on. In fact, this reaction force often receives it's own name, the ground reaction force.
• Similarly, a car accelerates forward because the road pushes forward on the drive wheels, in reaction to the drive wheels pushing backward on the ground. You can see evidence of the wheels pushing backward when tires spin on a gravel road and throw the rocks backward.
• Rockets move forward by expelling gas backward at high velocity. This means the rocket exerts a large backward force on the gas in the rocket combustion chamber; therefore, the gas exerts a large reaction force forward on the rocket. Although not often examined in biomechanics, this reaction force, which pushes a body forward in response to a backward force, is called thrust. It is a common misconception that rockets propel themselves by pushing on the ground or on the air behind them. They actually work better in a vacuum, where they can more readily expel the exhaust gases.
• Helicopters create lift by pushing air down, thereby experiencing an upward reaction force.
• Birds and airplanes also fly by exerting force on the air in a direction opposite that of whatever force they need. For example, the wings of a bird force air downward and backward to get lift and move forward.
• An octopus propels itself in the water by ejecting water through a funnel from its body, similar to a jet ski.
• When a person pulls down on a vertical rope, the rope pulls up on the person (Figure 4.17).

There are two important features of Newton’s third law. First, the forces exerted (the action and reaction) are always equal in magnitude but opposite in direction. Second, these forces are acting on different bodies or systems: A’s force acts on B and B’s force acts on A. In other words, the two forces are distinct forces that do not act on the same body. Thus, they do not cancel each other.

For the situation shown in Figure 4.6, the third law indicates that because the chair is pushing upward on the boy with force [latex]\overset{\to }{C},[/latex] he is pushing downward on the chair with force [latex]\text{−}\overset{\to }{C}.[/latex] Similarly, he is pushing downward with forces [latex]\text{−}\overset{\to }{F}[/latex] and [latex]\text{−}\overset{\to }{T}[/latex] on the floor and table, respectively. Finally, since Earth pulls downward on the boy with force [latex]\overset{\to }{w},[/latex] he pulls upward on Earth with force [latex]\text{−}\overset{\to }{w}[/latex]. If that student were to angrily pound the table in frustration, they would quickly learn the painful lesson (avoidable by studying Newton’s laws) that the table hits back just as hard.

A person who is walking or running applies Newton’s third law instinctively. For example, the runner in Figure 4.18 pushes backward on the ground so that it pushes him forward.

Example: Visualizing Reaction Forces on Stationary Objects

The package in Figure 4.19 is sitting on a scale. The forces on the package are [latex]\overset{\to }{S},[/latex] which is due to the scale, and [latex]\text{−}\overset{\to }{w},[/latex] which is due to Earth’s gravitational field. The reaction forces that the package exerts are [latex]\text{−}\overset{\to }{S}[/latex] on the scale and [latex]\overset{\to }{w}[/latex] on Earth. Because the package is not accelerating,

[latex]\sum F = 0 = {S} +\overset{\to }{w}= {0},[/latex]

so

[latex]\overset{\to }{S}=-\overset{\to }{w}[/latex]

Thus, the scale reading gives the magnitude of the package’s weight. However, the scale does not measure the weight of the package; it measures the force [latex]\text{−}\overset{\to }{S}[/latex] on its surface.

 

Example: Choosing the Correct System

A physics professor pushes a cart of demonstration equipment to a lecture hall (Figure 4.20). Her mass is 65.0 kg, the cart’s mass is 12.0 kg, and the equipment’s mass is 7.0 kg. Calculate the acceleration produced when the professor exerts a backward force of 150 N on the floor. All forces opposing the motion, such as friction on the cart’s wheels and air resistance, total 24.0 N.

Strategy

Since they accelerate as a unit, we define the system to be the professor, cart, and equipment, as seen in Figure 4.20. The professor pushes backward with a force [latex]{F}_{\text{foot}}[/latex] of 150 N. According to Newton’s third law, the floor exerts a forward reaction force [latex]{F}_{\text{floor}}[/latex] of 150 N.

Because all motion is horizontal, we can assume there is no net force in the vertical direction. Therefore, the problem is one-dimensional along the horizontal direction. As noted, friction f opposes the motion and is thus in the opposite direction of [latex]{F}_{\text{floor}}.[/latex] We do not include the forces [latex]{F}_{\text{prof}}[/latex] or [latex]{F}_{\text{cart}}[/latex] because these are internal forces, and we do not include [latex]{F}_{\text{foot}}[/latex] because it acts on the floor, not on the system. There are no other significant forces acting on the system (System 1 in Figure 4.20).

If the net external force can be found from all this information, we can use Newton’s second law to find the acceleration as requested. See the free-body diagram in the figure.

Solution

Newton’s second law is given by

[latex]a=\frac{{F}_{\text{net}}}{m}.[/latex]

The net external force on System 1 is deduced from Figure 4.20 and the preceding discussion to be:

[latex]{F}_{\text{net}}={F}_{\text{floor}}-f=150\,\text{N}-24.0\,\text{N}=126\,\text{N}\text{.}[/latex]

The mass of System 1 is

[latex]m=(65.0+12.0+7.0)\,\text{kg}=84\,\text{kg}\text{.}[/latex]

These values of [latex]{F}_{\text{net}} [latex] and m produce an acceleration of

[latex]a=\frac{{F}_{\text{net}}}{m}=\frac{126\,\text{N}}{84\,\text{kg}}=1.5\,{\text{m/s}}^{2}.[/latex]

 

Discussion

None of the forces between components of System 1, such as between the professor’s hands and the cart, contribute to the net external force because they are internal to System 1. Another way to look at this is that forces between components of a system cancel because they are equal in magnitude and opposite in direction. For example, the force exerted by the professor on the cart results in an equal and opposite force back on the professor. In this case, both forces act on the same system and therefore cancel. Thus, internal forces (between components of a system) cancel. Choosing System 1 was crucial to solving this problem.