By the end of the section, you will be able to:
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.
Whenever one body exerts a force on a second body, the first body experiences a force that is equal in magnitude and opposite in direction to the force that it exerts. Mathematically, if a body A exerts a force [latex] \overset{\to }{F} [/latex] on body B, then B simultaneously exerts a force [latex] \text{−}\overset{\to }{F} [/latex] on A, or in vector equation form, [latex] {\overset{\to }{F}}_{\text{AB}}=\text{−}{\overset{\to }{F}}_{\text{BA}}. [/latex] Newton’s third law represents a certain symmetry in nature: Forces always occur in pairs, and one body cannot exert a force on another without experiencing a force itself. We sometimes refer to this law loosely as “action-reaction,” where the force exerted is the action and the force experienced as a consequence is the reaction. Newton’s third law has practical uses in analyzing the origin of forces and understanding which forces are external to a system. 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)). 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), 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:
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), 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, he 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) pushes backward on the ground so that it pushes him forward.
The package in (Figure) 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, application of the second law yields [latex] \overset{\to }{S}-\overset{\to }{w}=m\overset{\to }{a}=\overset{\to }{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. If the system is accelerating, [latex] \overset{\to }{S} [/latex] and [latex] \text{−}\overset{\to }{w} [/latex] would not be equal, as explained in Applications of Newton’s Laws.
A physics professor pushes a cart of demonstration equipment to a lecture hall ((Figure)). 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. StrategySince they accelerate as a unit, we define the system to be the professor, cart, and equipment. This is System 1 in (Figure). 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 on System 1. 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 System 1. 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. SolutionNewton’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) 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] 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.
Calculate the force the professor exerts on the cart in (Figure), using data from the previous example if needed. StrategyIf we define the system of interest as the cart plus the equipment (System 2 in (Figure)), then the net external force on System 2 is the force the professor exerts on the cart minus friction. The force she exerts on the cart, [latex] {F}_{\text{prof}} [/latex], is an external force acting on System 2. [latex] {F}_{\text{prof}} [/latex] was internal to System 1, but it is external to System 2 and thus enters Newton’s second law for this system. SolutionNewton’s second law can be used to find [latex] {F}_{\text{prof}}. [/latex] We start with [latex] a=\frac{{F}_{\text{net}}}{m}. [/latex] The magnitude of the net external force on System 2 is [latex] {F}_{\text{net}}={F}_{\text{prof}}-f. [/latex] We solve for [latex] {F}_{\text{prof}} [/latex], the desired quantity: [latex] {F}_{\text{prof}}={F}_{\text{net}}+f. [/latex] The value of f is given, so we must calculate net [latex] {F}_{\text{net}}. [/latex] That can be done because both the acceleration and the mass of System 2 are known. Using Newton’s second law, we see that [latex] {F}_{\text{net}}=ma, [/latex] where the mass of System 2 is 19.0 kg ([latex] m=12.0\,\text{kg}+7.0\,\text{kg} [/latex]) and its acceleration was found to be [latex] a=1.5\,{\text{m/s}}^{2} [/latex] in the previous example. Thus, [latex] {F}_{\text{net}}=ma=(19.0\,\text{kg})(1.5\,{\text{m/s}}^{2})=29\,\text{N}\text{.} [/latex] Now we can find the desired force: [latex] {F}_{\text{prof}}={F}_{\text{net}}+f=29\,\text{N}+24.0\,\text{N}=53\,\text{N}\text{.} [/latex] This force is significantly less than the 150-N force the professor exerted backward on the floor. Not all of that 150-N force is transmitted to the cart; some of it accelerates the professor. The choice of a system is an important analytical step both in solving problems and in thoroughly understanding the physics of the situation (which are not necessarily the same things).
Two blocks are at rest and in contact on a frictionless surface as shown below, with [latex] {m}_{1}=2.0\,\text{kg}, [/latex] [latex] {m}_{2}=6.0\,\text{kg}, [/latex] and applied force 24 N. (a) Find the acceleration of the system of blocks. (b) Suppose that the blocks are later separated. What force will give the second block, with the mass of 6.0 kg, the same acceleration as the system of blocks?
View this video to watch examples of action and reaction.
View this video to watch examples of Newton’s laws and internal and external forces. Summary
Identify the action and reaction forces in the following situations: (a) Earth attracts the Moon, (b) a boy kicks a football, (c) a rocket accelerates upward, (d) a car accelerates forward, (e) a high jumper leaps, and (f) a bullet is shot from a gun.
Suppose that you are holding a cup of coffee in your hand. Identify all forces on the cup and the reaction to each force.
(a) Why does an ordinary rifle recoil (kick backward) when fired? (b) The barrel of a recoilless rifle is open at both ends. Describe how Newton’s third law applies when one is fired. (c) Can you safely stand close behind one when it is fired?
(a) What net external force is exerted on a 1100.0-kg artillery shell fired from a battleship if the shell is accelerated at [latex] 2.40\,×\,{10}^{4}\,{\text{m/s}}^{2}? [/latex] (b) What is the magnitude of the force exerted on the ship by the artillery shell, and why?
A brave but inadequate rugby player is being pushed backward by an opposing player who is exerting a force of 800.0 N on him. The mass of the losing player plus equipment is 90.0 kg, and he is accelerating backward at [latex] 1.20\,{\text{m/s}}^{2} [/latex]. (a) What is the force of friction between the losing player’s feet and the grass? (b) What force does the winning player exert on the ground to move forward if his mass plus equipment is 110.0 kg?
A history book is lying on top of a physics book on a desk, as shown below; a free-body diagram is also shown. The history and physics books weigh 14 N and 18 N, respectively. Identify each force on each book with a double subscript notation (for instance, the contact force of the history book pressing against physics book can be described as [latex] {\overset{\to }{F}}_{\text{HP}} [/latex]), and determine the value of each of these forces, explaining the process used.
A truck collides with a car, and during the collision, the net force on each vehicle is essentially the force exerted by the other. Suppose the mass of the car is 550 kg, the mass of the truck is 2200 kg, and the magnitude of the truck’s acceleration is [latex] 10\,{\text{m/s}}^{2} [/latex]. Find the magnitude of the car’s acceleration. Newton’s third law of motion whenever one body exerts a force on a second body, the first body experiences a force that is equal in magnitude and opposite in direction to the force that it exerts thrust reaction force that pushes a body forward in response to a backward force |