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Conservative Forces and Potential Energy

Module by: OpenStax College. E-mail the author

Summary:

  • Define conservative force, potential energy, and mechanical energy.
  • Explain the potential energy of a spring in terms of its compression when Hooke’s law applies.
  • Use the work-energy theorem to show how having only conservative forces implies conservation of mechanical energy.
  • Apply conservation of mechanical energy to solve mechanics problems in terms of potential energies instead of forces.

Note: You are viewing an old version of this document. The latest version is available here.

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)(PE) size 12{ \( "PE" \) } {} 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 and Conservative Forces:

Potential energy is the energy a system has due to position, shape, or configuration. It is stored energy that is completely recoverable.

A conservative force is one 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)(PE) size 12{ \( "PE" \) } {} for any conservative force. The work done against a conservative force to reach a final configuration depends on the configuration, not the path followed, and is the potential energy added.

Potential Energy of a Spring

First, let us obtain an expression for the potential energy stored in a spring (PEsPEs size 12{"PE" rSub { size 8{s} } } {}). 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 FF size 12{F} {} on the spring and the resulting deformation ΔLΔL size 12{ΔL} {} are proportional, F=kΔLF=kΔL size 12{F=kΔL} {}.) (See Figure 1.) For our spring, we will replace ΔLΔL (the amount of deformation produced by a force FF) by the distance xx that the spring is stretched or compressed along its length. So the force needed to stretch the spring has magnitude F = kxF = kx size 12{ ital "F = kx"} {}, where kk size 12{k} {} is the spring’s force constant. The force increases linearly from 0 at the start to kxkx size 12{ ital "kx"} {} in the fully stretched position. The average force is kx/2kx/2. Thus the work done in stretching or compressing the spring is Ws=Fd=kx2x=12kx2Ws=Fd=kx2x=12kx2 size 12{W rSub { size 8{s} } = ital "Fd"= left ( { { ital "kx"} over {2} } right )""x= { {1} over {2} } ital "kx" rSup { size 8{2} } } {}. Alternatively, we noted in Kinetic Energy and the Work-Energy Theorem that the area under a graph of FF size 12{F} {} vs. xx size 12{x} {} is the work done by the force. In Figure 1(c) we see that this area is also 12kx212kx2 size 12{ { {1} over {2} } ital "kx" rSup { size 8{2} } } {}. We therefore define the potential energy of a spring, PEsPEs size 12{"PE" rSub { size 8{s} } } {}, to be

PEs=12kx2,PEs=12kx2, size 12{"PE" rSub { size 8{s} } = { {1} over {2} } ital "kx" rSup { size 8{2} } } {}
(1)

where kk size 12{k} {} is the spring’s force constant and xx size 12{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 xx size 12{x} {}. The potential energy of the spring PEsPEs size 12{"PE" rSub { size 8{s} } } {} does not depend on the path taken; it depends only on the stretch or squeeze xx size 12{x} {} in the final configuration.

Figure 1: (a) An undeformed spring has no PEsPEs size 12{"PE" rSub { size 8{s} } } {} stored in it. (b) The force needed to stretch (or compress) the spring a distance xx size 12{x} {} has a magnitude F=kxF=kx size 12{F= ital "kx"} {} , and the work done to stretch (or compress) it is 12kx212kx2 size 12{ { {1} over {2} } ital "kx" rSup { size 8{2} } } {}. Because the force is conservative, this work is stored as potential energy (PEs)(PEs) size 12{ \( "PE" rSub { size 8{s} } \) } {} in the spring, and it can be fully recovered. (c) A graph of FF size 12{F} {} vs. xx size 12{x} {} has a slope of kk size 12{k} {}, and the area under the graph is 12kx212kx2 size 12{ { {1} over {2} } ital "kx" rSup { size 8{2} } } {}. Thus the work done or potential energy stored is 12kx212kx2.
An undeformed spring fixed at one end with no potential energy. (b) A spring fixed at one end and stretched by a distance x by a force F equal to k x. Work done W is equal to one half k x squared. P E s is equal to one half k x squared. (c) A graph of force F versus elongation x in the spring. A straight line inclined to x axis starts from origin. The area under this line forms a right triangle with base of x and height of k x. Area of this triangle is equal to one half k x squared.

The equation PEs=12kx2PEs=12kx2 size 12{"PE" rSub { size 8{s} } = { {1} over {2} } ital "kx" rSup { size 8{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 PEs=12kx2PEs=12kx2 size 12{"PE" rSub { size 8{s} } = { {1} over {2} } ital "kx" rSup { size 8{2} } } {}, where kk size 12{k} {} is the force constant of the particular system and xx size 12{x} {} is its deformation. Another example is seen in Figure 2 for a guitar string.

Figure 2: 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.
A six-string guitar is placed vertically. The left-most string is plucked in the left direction with a force F shown by an arrow pointing left. The displacement of the string from the mean position is d. The plucked string is labeled P E sub string, to represent the potential energy of 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 net = 1 2 mv 2 1 2 mv 0 2 = Δ KE. W net = 1 2 mv 2 1 2 mv 0 2 = Δ KE. size 12{W rSub { size 8{"net"} } = { {1} over {2} } ital "mv" rSup { size 8{2} } - { {1} over {2} } ital "mv" rSub { size 8{0} rSup { size 8{2} } } =Δ"KE" "." } {}
(2)

If only conservative forces act, then

Wnet=Wc,Wnet=Wc, size 12{W rSub { size 8{"net"} } =W rSub { size 8{c} } } {}
(3)

where WcWc is the total work done by all conservative forces. Thus,

Wc=ΔKE.Wc=ΔKE. size 12{W rSub { size 8{c} } =Δ"KE"} {}
(4)

Now, if the conservative force, such as the gravitational force or a spring force, does work, the system loses potential energy. That is, Wc=ΔPEWc=ΔPE size 12{W rSub { size 8{c} } = +- D"PE"} {}. Therefore,

Δ PE = Δ KE Δ PE = Δ KE size 12{ - Δ"PE"=Δ"KE"} {}
(5)

or

ΔKE+ΔPE=0.ΔKE+ΔPE=0. size 12{Δ"KE"+Δ"PE"=0} {}
(6)

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

KE + PE = constant     or KE i + PE i = KE f + PE f } (conservative forces only), KE + PE = constant     or KE i + PE i = KE f + PE f } (conservative forces only),
(7)

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)(KE+PE) size 12{ \( "KE"+"PE" \) } {}. In a system that experiences only conservative forces, there is a potential energy associated with each force, and the energy only changes form between KEKE size 12{"KE"} {} and the various types of PEPE size 12{"PE"} {}, with the total energy remaining constant.

Example 1: Using Conservation of Mechanical Energy to Calculate the Speed of a Toy Car

A 0.100-kg toy car is propelled by a compressed spring, as shown in Figure 3. The car follows a track that rises 0.180 m above the starting point. The spring is compressed 4.00 cm and has a force constant of 250.0 N/m. Assuming work done by friction to be negligible, find (a) how fast the car is going before it starts up the slope and (b) how fast it is going at the top of the slope.

Figure 3: A toy car is pushed by a compressed spring and coasts up a slope. Assuming negligible friction, the potential energy in the spring is first completely converted to kinetic energy, and then to a combination of kinetic and gravitational potential energy as the car rises. The details of the path are unimportant because all forces are conservative—the car would have the same final speed if it took the alternate path shown.
The figure shows a toy race car that has just been released from a spring. Two possible paths for the car are shown. One path has a gradual upward incline, leveling off at a height of eighteen centimeters above its starting level. An alternative path shows the car descending from its starting point, making a loop, and then ascending back up and leveling off at a height of eighteen centimeters above its starting level.

Strategy

The spring force and the gravitational force are conservative forces, so conservation of mechanical energy can be used. Thus,

KE i + PE i = KE f + PE f KE i + PE i = KE f + PE f size 12{"KE""" lSub { size 8{i} } +"PE" rSub { size 8{i} } ="KE" rSub { size 8{f} } +"PE" rSub { size 8{f} } } {}
(8)

or

12 mvi2 + mgh i +12 kxi2 =12 mvf2+ mgh f + 12 kxf2, 12 mvi2 + mgh i +12 kxi2 =12 mvf2+ mgh f + 12 kxf2,
(9)

where hh size 12{h} {} is the height (vertical position) and xx size 12{x} {} is the compression of the spring. This general statement looks complex but becomes much simpler when we start considering specific situations. First, we must identify the initial and final conditions in a problem; then, we enter them into the last equation to solve for an unknown.

Solution for (a)

This part of the problem is limited to conditions just before the car is released and just after it leaves the spring. Take the initial height to be zero, so that both hihi size 12{h rSub { size 8{i} } } {} and hfhf size 12{h rSub { size 8{f} } } {} are zero. Furthermore, the initial speed vivi size 12{v rSub { size 8{i} } } {} is zero and the final compression of the spring xfxf size 12{x rSub { size 8{f} } } {} is zero, and so several terms in the conservation of mechanical energy equation are zero and it simplifies to

1 2 kx i 2 = 1 2 mv f 2 . 1 2 kx i 2 = 1 2 mv f 2 .
(10)

In other words, the initial potential energy in the spring is converted completely to kinetic energy in the absence of friction. Solving for the final speed and entering known values yields

v f = k m x i = 250 .0 N/m 0.100 kg ( 0.0400 m ) = 2.00 m/s. v f = k m x i = 250 .0 N/m 0.100 kg ( 0.0400 m ) = 2.00 m/s. alignl { stack { size 12{v rSub { size 8{f} } = sqrt { { {k} over {m} } } x rSub { size 8{i} } } {} # " "= sqrt { { {"250" "." 0" N/m"} over {0 "." "100 kg"} } } \( 0 "." "0400"" m" \) {} # " "=2 "." "00"" m/s" "." {} } } {}
(11)

Solution for (b)

One method of finding the speed at the top of the slope is to consider conditions just before the car is released and just after it reaches the top of the slope, completely ignoring everything in between. Doing the same type of analysis to find which terms are zero, the conservation of mechanical energy becomes

12 kxi 2 =1 2 mvf 2 +mghf.12 kxi 2 =1 2 mvf 2 +mghf. size 12{ { {1} over {2} } ital "kx" rSub { size 8{i} rSup { size 8{2} } } = { {1} over {2} } ital "mv" rSub { size 8{f} rSup { size 8{2} } } + ital "mgh" rSub { size 8{f} } } {}
(12)

This form of the equation means that the spring’s initial potential energy is converted partly to gravitational potential energy and partly to kinetic energy. The final speed at the top of the slope will be less than at the bottom. Solving for vfvf size 12{v rSub { size 8{f} } } {} and substituting known values gives

v f = kx i 2 m 2 gh f = 250.0 N/m 0.100 kg ( 0.0400 m ) 2 2 ( 9.80 m/s 2 ) ( 0.180 m ) = 0.687 m/s. v f = kx i 2 m 2 gh f = 250.0 N/m 0.100 kg ( 0.0400 m ) 2 2 ( 9.80 m/s 2 ) ( 0.180 m ) = 0.687 m/s. alignl { stack { size 12{v rSub { size 8{f} } = sqrt { { { ital "kx" rSub { size 8{i} rSup { size 8{2} } } } over {m} } - 2 ital "gh" rSub { size 8{f} } } } {} # " "= sqrt { left ( { {"250" "." 0" N/m"} over {0 "." "100 kg"} } right )"" \( 0 "." "0400"" m" \) rSup { size 8{2} } - 2 \( 9 "." "80"" m/s" rSup { size 8{2} } \) \( 0 "." "180"" m" \) } {} # " "=0 "." "687"" m/s" "." {} } } {}
(13)

Discussion

Another way to solve this problem is to realize that the car’s kinetic energy before it goes up the slope is converted partly to potential energy—that is, to take the final conditions in part (a) to be the initial conditions in part (b).

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 1. 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.

PhET Explorations: Energy Skate Park:

Learn about conservation of energy with a skater dude! Build tracks, ramps and jumps for the skater and view the kinetic energy, potential energy and friction as he moves. You can also take the skater to different planets or even space!

Section Summary

  • A conservative force is one for which work depends only on the starting and ending points of a motion, not on the path taken.
  • We can define potential energy (PE)(PE) size 12{ \( "PE" \) } {} for any conservative force, just as we defined PEgPEg size 12{"PE" rSub { size 8{g} } } {} for the gravitational force.
  • The potential energy of a spring is PEs=12kx2PEs=12kx2 size 12{"PE" rSub { size 8{s} } = { {1} over {2} } ital "kx" rSup { size 8{2} } } {}, where kk size 12{k} {} is the spring’s force constant and xx size 12{x} {} is the displacement from its undeformed position.
  • Mechanical energy is defined to be KE + PEKE + PE size 12{"KE "+" PE"} {} for a conservative force.
  • When only conservative forces act on and within a system, the total mechanical energy is constant. In equation form,
KE + PE = constant     or KE i + PE i = KE f + PE f KE + PE = constant     or KE i + PE i = KE f + PE f (conservative forces only),
(14)

where i and f denote initial and final values. This is known as the conservation of mechanical energy.

Conceptual Questions

Exercise 1

What is a conservative force?

Exercise 2

The force exerted by a diving board is conservative, provided the internal friction is negligible. Assuming friction is negligible, describe changes in the potential energy of a diving board as a swimmer dives from it, starting just before the swimmer steps on the board until just after his feet leave it.

Exercise 3

Define mechanical energy. What is the relationship of mechanical energy to nonconservative forces? What happens to mechanical energy if only conservative forces act?

Exercise 4

What is the relationship of potential energy to conservative force?

Problems & Exercises

Exercise 1

A 5.00×105-kg5.00×105-kg size 12{5 "." "00" times "10" rSup { size 8{5} } "-kg"} {} subway train is brought to a stop from a speed of 0.500 m/s in 0.400 m by a large spring bumper at the end of its track. What is the force constant kk size 12{k} {} of the spring?

Solution

7.81 × 10 5 N/m 7.81 × 10 5 N/m size 12{7 "." "81" times "10" rSup { size 8{5} } " N/m"} {}
(15)

Exercise 2

A pogo stick has a spring with a force constant of 2.50×104 N/m2.50×104 N/m size 12{2 "." "50" times "10" rSup { size 8{4} } " N/m"} {}, which can be compressed 12.0 cm. To what maximum height can a child jump on the stick using only the energy in the spring, if the child and stick have a total mass of 40.0 kg? Explicitly show how you follow the steps in the Problem-Solving Strategies for Energy.

Glossary

conservative force:
a force that does the same work for any given initial and final configuration, regardless of the path followed
potential energy:
energy due to position, shape, or configuration
potential energy of a spring:
the stored energy of a spring as a function of its displacement; when Hooke’s law applies, it is given by the expression 12kx212kx2 size 12{ { {1} over {2} } ital "kx" rSup { size 8{2} } } {} where xx size 12{x} {} is the distance the spring is compressed or extended and kk size 12{k} {} is the spring constant
conservation of mechanical energy:
the rule that the sum of the kinetic energies and potential energies remains constant if only conservative forces act on and within a system
mechanical energy:
the sum of kinetic energy and potential energy

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