Conservative Forces and Potential Energy

Potential Energy and Conservative Forces

Work is done by a force, and some forces, such as weight, have special characteristics. A conservative force is one, like the gravitational force, for which work done by or against it depends only on the starting and ending points of a motion and not on the path taken. We can define a potential energy $(PE)$ for any conservative force, just as we did for the gravitational force. 

For example, when you wind up a toy, an egg timer, or an old-fashioned watch, you do work against its spring and store energy in it. (We treat these springs as ideal, in that we assume there is no friction and no production of thermal energy.) This stored energy is recoverable as work, and it is useful to think of it as potential energy contained in the spring. Indeed, the reason that the spring has this characteristic is that its force is conservative. That is, a conservative force results in stored or potential energy. Gravitational potential energy is one example, as is the energy stored in a spring. We will also see how conservative forces are related to the conservation of energy.

Potential Energy of a Spring

First, let us obtain an expression for the potential energy stored in a spring $(PEs)$. We calculate the work done to stretch or compress a spring that obeys Hooke's law. (Hooke's law was examined in Elasticity: Stress and Strain, and states that the magnitude of force $F$ on the spring and the resulting deformation $\Delta L$ are proportional, $F=k \Delta L$.) (See Figure 7.10.) For our spring, we will replace $\Delta L$ (the amount of deformation produced by a force $F$) by the distance $x$ that the spring is stretched or compressed along its length.

So the force needed to stretch the spring has magnitude $F=k x$, where $k$ is the spring's force constant. The force increases linearly from 0 at the start to $kx$ in the fully stretched position. The average force is $kx/2$. Thus the work done in stretching or compressing the spring is $W_{\mathrm{s}}=F d=\left(\frac{k x}{2}\right) x=\frac{1}{2} k x^{2}$. Alternatively, we noted in Kinetic Energy and the Work-Energy Theorem that the area under a graph of $F$ vs. $x$ is the work done by the force. In Figure 7.10(c) we see that this area is also $\frac{1}{2} k x^{2}$. We therefore define the potential energy of a spring, $PEs$, to be

$\mathrm{PE}_{\mathrm{s}}=\frac{1}{2} k x^{2}$,

where $k$ is the spring's force constant and $x$ is the displacement from its undeformed position. The potential energy represents the work done on the spring and the energy stored in it as a result of stretching or compressing it a distance $x$. The potential energy of the spring $PEs$ does not depend on the path taken; it depends only on the stretch or squeeze x in the final configuration.

Figure 7.10 (a) An undeformed spring has no $PEs$ stored in it. (b) The force needed to stretch (or compress) the spring a distance $x$ has a magnitude $F=kx$ , and the work done to stretch (or compress) it is $\frac{1}{2} k x^{2}$. Because the force is conservative, this work is stored as potential energy $(PEs)$ in the spring, and it can be fully recovered. (c) A graph of $F$ vs. $x$ has a slope of $k$ , and the area under the graph is $\frac{1}{2} k x^{2}$. Thus the work done or potential energy stored is $\frac{1}{2} k x^{2}$.

The equation $\mathrm{PE}_{\mathrm{s}}=\frac{1}{2} k x^{2}$ has general validity beyond the special case for which it was derived. Potential energy can be stored in any elastic medium by deforming it. Indeed, the general definition of potential energy is energy due to position, shape, or configuration. For shape or position deformations, stored energy is $\mathrm{PE}_{\mathrm{s}}=\frac{1}{2} k x^{2}$, where $k$ is the force constant of the particular system and $x$ is its deformation. Another example is seen in Figure 7.11 for a guitar string.

Figure 7.11 Work is done to deform the guitar string, giving it potential energy. When released, the potential energy is converted to kinetic energy and back to potential as the string oscillates back and forth. A very small fraction is dissipated as sound energy, slowly removing energy from the string.

Conservation of Mechanical Energy

Let us now consider what form the work-energy theorem takes when only conservative forces are involved. This will lead us to the conservation of energy principle. The work-energy theorem states that the net work done by all forces acting on a system equals its change in kinetic energy. In equation form, this is

$W_{\mathrm{net}}=\frac{1}{2} m v^{2}-\frac{1}{2} m v_{0}^{2}=\Delta \mathrm{KE}$.

If only conservative forces act, then

$W_{\text {net }}=W_{\mathrm{c}}$,

where $W_{\mathrm{c}}$ is the total work done by all conservative forces. Thus,

$W_{\mathrm{c}}=\Delta \mathrm{KE}$.

Now, if the conservative force, such as the gravitational force or a spring force, does work, the system loses potential energy. That is, $W_{\mathrm{c}}=-\Delta \mathrm{PE}$. Therefore,

$-\Delta \mathrm{PE}=\Delta \mathrm{KE}$

or

$\Delta \mathrm{KE}+\Delta \mathrm{PE}=0$.

This equation means that the total kinetic and potential energy is constant for any process involving only conservative forces. That is,

$\begin{aligned} &\text { or } \left.\begin{array}{l} \mathrm{KE}+\mathrm{PE}=\mathrm{constant} \\ \mathrm{KE}_{\mathrm{i}}+\mathrm{PE}_{\mathrm{i}}=\mathrm{KE}_{\mathrm{f}}+\mathrm{PE}_{\mathrm{f}} \end{array}\right\} \text { (conservative forces only), } \end{aligned}$

where i and f denote initial and final values. This equation is a form of the work-energy theorem for conservative forces; it is known as the conservation of mechanical energy principle. Remember that this applies to the extent that all the forces are conservative, so that friction is negligible. The total kinetic plus potential energy of a system is defined to be its mechanical energy, $(KE+PE)$. In a system that experiences only conservative forces, there is a potential energy associated with each force, and the energy only changes form between $KE$ and the various types of $PE$, with the total energy remaining constant.

Note that, for conservative forces, we do not directly calculate the work they do; rather, we consider their effects through their corresponding potential energies, just as we did in Example 7.8. Note also that we do not consider details of the path taken – only the starting and ending points are important (as long as the path is not impossible). This assumption is usually a tremendous simplification, because the path may be complicated and forces may vary along the way.

Source: Rice University, https://openstax.org/books/college-physics/pages/7-4-conservative-forces-and-potential-energy
This work is licensed under a Creative Commons Attribution 4.0 License.