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It seems reasonable that acceleration would be directly proportional to and in the same direction as the net external force acting on a system. This assumption has been verified experimentally and is illustrated in [link] . To obtain an equation for Newton’s second law, we first write the relationship of acceleration a and net external force F net as the proportionality

a F net

where the symbol means “proportional to.” (Recall from Forces that the net external force is the vector sum of all external forces and is sometimes indicated as F . ) This proportionality shows what we have said in words—acceleration is directly proportional to net external force. Once the system of interest is chosen, identify the external forces and ignore the internal ones. It is a tremendous simplification to disregard the numerous internal forces acting between objects within the system, such as muscular forces within the students’ bodies, let alone the myriad forces between the atoms in the objects. Still, this simplification helps us solve some complex problems.

It also seems reasonable that acceleration should be inversely proportional to the mass of the system. In other words, the larger the mass (the inertia), the smaller the acceleration produced by a given force. As illustrated in [link] , the same net external force applied to a basketball produces a much smaller acceleration when it is applied to an SUV. The proportionality is written as

a 1 m ,

where m is the mass of the system and a is the magnitude of the acceleration. Experiments have shown that acceleration is exactly inversely proportional to mass, just as it is directly proportional to net external force.

Figure a shows a person exerting force F on a basketball with mass m1. The ball is shown to move to the rigth with an acceleration a1. Figure b shows the person exerting the same amount of force, F on an SUV with mass m2. The acceleration is a2, which is much smaller than a1. Figure c shows the free body diagrams of both systems shown in figure a and figure b. Both show the force F having the same magnitude and direction. The label reads: the free-body diagrams of both objects are the same.
The same force exerted on systems of different masses produces different accelerations. (a) A basketball player pushes on a basketball to make a pass. (Ignore the effect of gravity on the ball.) (b) The same player exerts an identical force on a stalled SUV and produces far less acceleration. (c) The free-body diagrams are identical, permitting direct comparison of the two situations. A series of patterns for free-body diagrams will emerge as you do more problems and learn how to draw them in Drawing Free-Body Diagrams .

It has been found that the acceleration of an object depends only on the net external force and the mass of the object. Combining the two proportionalities just given yields Newton’s second law .

Newton’s second law of motion

The acceleration of a system is directly proportional to and in the same direction as the net external force acting on the system and is inversely proportion to its mass. In equation form, Newton’s second law is

a = F net m ,

where a is the acceleration, F net is the net force, and m is the mass. This is often written in the more familiar form

F net = F = m a ,

but the first equation gives more insight into what Newton’s second law means. When only the magnitude of force and acceleration are considered, this equation can be written in the simpler scalar form:

F net = m a .

The law is a cause-and-effect relationship among three quantities that is not simply based on their definitions. The validity of the second law is based on experimental verification. The free-body diagram, which you will learn to draw in Drawing Free-Body Diagrams , is the basis for writing Newton’s second law.

Practice Key Terms 1

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Source:  OpenStax, University physics volume 1. OpenStax CNX. Sep 19, 2016 Download for free at http://cnx.org/content/col12031/1.5
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