Learning Objectives

Learning Objectives

By the end of this section, you will be able to do the following:

  • Define and discuss binding energy
  • Calculate the binding energy per nucleon of a particle

The information presented in this section supports the following AP® learning objectives and science practices:

  • 3.G.3.1 The student is able to identify the strong force as the force that is responsible for holding the nucleus together.

The more tightly bound a system is, the stronger the forces that hold it together and the greater the energy required to pull it apart. We can therefore learn about nuclear forces by examining how tightly bound the nuclei are. We define the binding energy (BE) of a nucleus to be the energy required to completely disassemble it into separate protons and neutrons. We can determine the BE of a nucleus from its rest mass. The two are connected through Einstein’s famous relationship E=(Δm)c2.E=(Δm)c2. size 12{E= \( Δm \) c rSup { size 8{2} } } {} A bound system has a smaller mass than its separate constituents; the more tightly the nucleons are bound together, the smaller the mass of the nucleus.

Imagine pulling a nuclide apart as illustrated in Figure 14.19. Work done to overcome the nuclear forces holding the nucleus together puts energy into the system. By definition, the energy input equals the binding energy BE. The pieces are at rest when separated, and so the energy put into them increases their total rest mass compared with what it was when they were glued together as a nucleus. That mass increase is thus Δm=BE/c2.Δm=BE/c2. size 12{Δm="BE"/c rSup { size 8{2} } } {} This difference in mass is known as mass defect. It implies that the mass of the nucleus is less than the sum of the masses of its constituent protons and neutrons. A nuclide AXAX size 12{"" lSup { size 8{A} } X} {} has ZZ size 12{Z} {} protons and NN size 12{N} {} neutrons, so that the difference in mass is

14.60 Δm=(Zmp+Nmn)mtot.Δm=(Zmp+Nmn)mtot. size 12{Δm= \( ital "Zm" rSub { size 8{p} } + ital "Nm" rSub { size 8{n} } \) - m rSub { size 8{"tot"} } } {}

Thus,

14.61 BE=(Δm)c2=[(Zmp+Nmn)mtot]c2,BE=(Δm)c2=[(Zmp+Nmn)mtot]c2, size 12{"BE"= \( Δm \) c rSup { size 8{2} } = \[ \( ital "Zm" rSub { size 8{p} } + ital "Nm" rSub { size 8{n} } \) - m rSub { size 8{"tot"} } \] c rSup { size 8{2} } } {}

where mtotmtot size 12{m rSub { size 8{"tot"} } } {} is the mass of the nuclide AX,AX, mpmp is the mass of a proton, and mnmn is the mass of a neutron. Traditionally, we deal with the masses of neutral atoms. To get atomic masses into the last equation, we first add ZZ size 12{Z} {} electrons to mtot,mtot, size 12{m rSub { size 8{"tot"} } } {} which gives mAX,mAX, size 12{m left ("" lSup { size 8{A} } X right )} {} the atomic mass of the nuclide. We then add ZZ size 12{Z} {} electrons to the ZZ size 12{Z} {} protons, which gives Zm1H,Zm1H, size 12{ ital "Zm" left ("" lSup { size 8{1} } H right )} {} or ZZ size 12{Z} {} times the mass of a hydrogen atom. Thus the binding energy of a nuclide AXAX size 12{"" lSup { size 8{A} } X} {} is

14.62 BE = { [ Zm ( 1 H ) + Nm n ] m ( A X )} c 2 . BE = { [ Zm ( 1 H ) + Nm n ] m ( A X )} c 2 .

The atomic masses can be found in Exercise 17.31, most conveniently expressed in unified atomic mass units u (1u=931.5MeV/c2).(1u=931.5MeV/c2). size 12{1" u"="931" "." 5 "MeV"/c rSup { size 8{2} } } {} BE is thus calculated from known atomic masses.

The image shows some spherical protons and neutrons pulled out from a nucleus. The work done to pull them apart is binding energy.
Figure 14.19 Work done to pull a nucleus apart into its constituent protons and neutrons increases the mass of the system. The work to disassemble the nucleus equals its binding energy BE. A bound system has less mass than the sum of its parts, especially noticeable in the nuclei, where forces and energies are very large.

Things Great and Small

Nuclear Decay Helps Explain Earth’s Hot Interior

A puzzle created by radioactive dating of rocks is resolved by radioactive heating of Earth’s interior. This intriguing story is another example of how small-scale physics can explain large-scale phenomena.

Radioactive dating plays a role in determining the approximate age of Earth. The oldest rocks on Earth solidified about 3.5×1093.5×109 size 12{3 "." 5 times "10" rSup { size 8{9} } } {} years ago—a number determined by uranium-238 dating. These rocks could only have solidified once the surface of Earth had cooled sufficiently. The temperature of Earth at formation can be estimated based on gravitational potential energy of the assemblage of pieces being converted to thermal energy. Using heat transfer concepts discussed in Thermodynamics, it is then possible to calculate how long it would take for the surface to cool to rock-formation temperatures. The result is about 109109 size 12{"10" rSup { size 8{9} } } {} years. The first rocks formed have been solid for 3.5×1093.5×109 size 12{3 "." 5 times "10" rSup { size 8{9} } } {} years, so that the age of Earth is approximately 4.5×1094.5×109 size 12{4 "." 5 times "10" rSup { size 8{9} } } {} years. There is a large body of other types of evidence—both Earth-bound and solar system characteristics are used—that supports this age. The puzzle is that, given its age and initial temperature, the center of Earth should be much cooler than it is today (see Figure 14.20).

The figure shows that the center of the Earth cools by three heat transfer methods. Convection heat transfer in the center region, then conduction heat transfer moves thermal energy to the surface, and finally radiation heat transfer from the surface to space.
Figure 14.20 The center of Earth cools by well-known heat transfer methods. Convection in the liquid regions and conduction move thermal energy to the surface, where it radiates into cold, dark space. Given the age of Earth and its initial temperature, it should have cooled to a lower temperature by now. The blowup shows that nuclear decay releases energy in Earth’s interior. This energy has slowed the cooling process and is responsible for the interior still being molten.

We know from seismic waves produced by earthquakes that parts of the interior of Earth are liquid. Shear or transverse waves cannot travel through a liquid and are not transmitted through Earth’s core. Yet compression or longitudinal waves can pass through a liquid and do go through the core. From this information, the temperature of the interior can be estimated. As noticed, the interior should have cooled more from its initial temperature in the 4.5×1094.5×109 size 12{4 "." 5 times "10" rSup { size 8{9} } } {} years since its formation. In fact, it should have taken no more than about 109109 size 12{4 "." 5 times "10" rSup { size 8{9} } } {} years to cool to its present temperature. What is keeping it hot? The answer seems to be radioactive decay of primordial elements that were part of the material that formed Earth (see the blowup in Figure 14.20).

Nuclides such as 238U238U and 40K40K have half-lives similar to or longer than the age of Earth, and their decay still contributes energy to the interior. Some of the primordial radioactive nuclides have unstable decay products that also release energy—238U238U size 12{"" lSup { size 8{"238"} } U} {} has a long decay chain of these. Further, there were more of these primordial radioactive nuclides early in the life of Earth, and thus the activity and energy contributed were greater then, perhaps by an order of magnitude. The amount of power created by these decays per cubic meter is very small. However, since a huge volume of material lies deep below the surface, this relatively small amount of energy cannot escape quickly. The power produced near the surface has much less distance to go to escape and has a negligible effect on surface temperatures.

A final effect of this trapped radiation merits mention. Alpha decay produces helium nuclei, which form helium atoms when they are stopped and capture electrons. Most of the helium on Earth is obtained from wells and is produced in this manner. Any helium in the atmosphere will escape in geologically short times because of its high thermal velocity.

What patterns and insights are gained from an examination of the binding energy of various nuclides? First, we find that BE is approximately proportional to the number of nucleons AA in any nucleus. About twice as much energy is needed to pull apart a nucleus like 24Mg24Mg compared with pulling apart 12C,12C, for example. To help us look at other effects, we divide BE by AA size 12{A} {} and consider the binding energy per nucleon, BE/A.BE/A. size 12{ {"BE"} slash {A} } {} The graph of BE/ABE/A size 12{ {"BE"} slash {A} } {} in Figure 14.21 reveals some very interesting aspects of nuclei. We see that the binding energy per nucleon averages about 8 MeV, but is lower for both the lightest and heaviest nuclei. This overall trend, in which nuclei with AA size 12{A} {} equal to about 60 have the greatest BE/ABE/A size 12{ {"BE"} slash {A} } {} and are thus the most tightly bound, is due to the combined characteristics of the attractive nuclear forces and the repulsive Coulomb force. It is especially important to note two things—the strong nuclear force is about 100 times stronger than the Coulomb force, and the nuclear forces are shorter in range compared to the Coulomb force. So, for low-mass nuclei, the nuclear attraction dominates and each added nucleon forms bonds with all others, causing progressively heavier nuclei to have progressively greater values of BE/A.BE/A. size 12{ {"BE"} slash {A} } {} This continues up to A60,A60, size 12{A approx "60"} {} roughly corresponding to the mass number of iron. Beyond that, new nucleons added to a nucleus will be too far from some others to feel their nuclear attraction. Added protons, however, feel the repulsion of all other protons, since the Coulomb force is longer in range. Coulomb repulsion grows for progressively heavier nuclei, but nuclear attraction remains about the same, and so BE/ABE/A size 12{ {"BE"} slash {A} } {} becomes smaller. This is why stable nuclei heavier than A40A40 size 12{A approx "40"} {} have more neutrons than protons. Coulomb repulsion is reduced by having more neutrons to keep the protons farther apart (see Figure 14.22).

The figure shows a graph of binding energy per nucleon versus atomic mass for different elements. From the graph it can be observed that elements with atomic mass near sixty have greater binding energy per nucleon.
Figure 14.21 A graph of average binding energy per nucleon, BE/A,BE/A, size 12{ {"BE"} slash {A} } {} for stable nuclei. The most tightly bound nuclei are those with AA size 12{A} {} near 60, where the attractive nuclear force has its greatest effect. At higher AA size 12{A} {}s, the Coulomb repulsion progressively reduces the binding energy per nucleon, because the nuclear force is short ranged. The spikes on the curve are very tightly bound nuclides and indicate shell closures.
The image shows a bunch of spherical nucleons inside a nucleus. A circular dashed path is shown which depicts the range of nuclear force and the nucleons inside that range feel nuclear force directly.
Figure 14.22 The nuclear force is attractive and stronger than the Coulomb force, but it is short ranged. In low-mass nuclei, each nucleon feels the nuclear attraction of all others. In larger nuclei, the range of the nuclear force, shown for a single nucleon, is smaller than the size of the nucleus, but the Coulomb repulsion from all protons reaches all others. If the nucleus is large enough, the Coulomb repulsion can add to overcome the nuclear attraction.

There are some noticeable spikes on the BE/ABE/A size 12{ {"BE"} slash {A} } {} graph, which represent particularly tightly bound nuclei. These spikes reveal further details of nuclear forces, such as confirming that closed-shell nuclei—those with magic numbers of protons or neutrons or both—are more tightly bound. The spikes also indicate that some nuclei with even numbers for ZZ size 12{Z} {} and N,N, size 12{N} {} and with Z=N,Z=N, size 12{Z=N} {} are exceptionally tightly bound. This finding can be correlated with some of the cosmic abundances of the elements. The most common elements in the universe, as determined by observations of atomic spectra from outer space, are hydrogen, followed by 4He,4He, with much smaller amounts of 12C12C and other elements. It should be noted that the heavier elements are created in supernova explosions, while the lighter ones are produced by nuclear fusion during the normal life cycles of stars, as will be discussed in subsequent chapters. The most common elements have the most tightly bound nuclei. It is also no accident that one of the most tightly bound light nuclei is 4He,4He, emitted in αα decay.

Example 14.7 What Is BE/ABE/A size 12{ {"BE"} slash {A} } {} for an Alpha Particle?

Calculate the binding energy per nucleon of 4He,4He, size 12{"" lSup { size 8{4} } "He"} {} the αα size 12{α} {}particle.

Strategy

To find BE/A,BE/A, we first find BE using the Equation BE={[Zm(1H)+Nmn]m(AX)}c2BE={[Zm(1H)+Nmn]m(AX)}c2 and then divide by A.A. This is straightforward once we have looked up the appropriate atomic masses in Exercise 17.31.

Solution

The binding energy for a nucleus is given by the equation

14.63 BE={[Zm(1H)+Nmn]m(AX)}c2.BE={[Zm(1H)+Nmn]m(AX)}c2.

For 4He,4He, size 12{"" lSup { size 8{4} } "He"} {} we have Z=N=2;Z=N=2; size 12{Z=N=2} {} thus,

14.64 BE={[2m(1H)+2mn]m(4He)}c2.BE={[2m(1H)+2mn]m(4He)}c2.

Exercise 17.31 gives these masses as m(4He)=4.002602 u,m(4He)=4.002602 u, m(1H)=1.007825 u,m(1H)=1.007825 u, and mn=1.008665 u.mn=1.008665 u. size 12{m rSub { size 8{n} } =0 "." "008665"`" u"} {} Thus

14.65 BE=(0.030378 u)c2.BE=(0.030378 u)c2. size 12{"BE"= \( 0 "." "030378 u" \) c rSup { size 8{2} } } {}

Noting that 1 u=931.5 MeV/c2,1 u=931.5 MeV/c2, size 12{"1u"="931" "." "5 MeV/"c rSup { size 8{2} } } {} we find

14.66 BE=(0.030378)(931.5 MeV/c2)c2=28.3 MeV.BE=(0.030378)(931.5 MeV/c2)c2=28.3 MeV. size 12{"BE"= \( 0 "." "030378" \) \( "931" "." "5 MeV/"c rSup { size 8{2} } \) c rSup { size 8{2} } ="28" "." 3" MeV"} {}

Since A=4,A=4, size 12{A=4} {} we see that BE/ABE/A size 12{ {"BE"} slash {A} } {} is this number divided by four, or

14.67 BE/A=7.07 MeV/nucleon.BE/A=7.07 MeV/nucleon. size 12{"BE"/A=7 "." "07"" MeV/nucleon"} {}

Discussion

This is a large binding energy per nucleon compared with those for other low-mass nuclei, which have BE/A3 MeV/nucleon.BE/A3 MeV/nucleon. This indicates that 4He4He is tightly bound compared with its neighbors on the chart of the nuclides. You can see the spike representing this value of BE/ABE/A for 4He4He on the graph in Figure 14.21. This is why 4He4He is stable. Since 4He4He is tightly bound, it has less mass than other A=4A=4 nuclei and, therefore, cannot spontaneously decay into them. The large binding energy also helps to explain why some nuclei undergo αα decay. Smaller mass in the decay products can mean energy release, and such decays can be spontaneous. Further, it can happen that two protons and two neutrons in a nucleus can randomly find themselves together, experience the exceptionally large nuclear force that binds this combination, and act as a 4He4He unit within the nucleus, at least for a while. In some cases, the 4He4He escapes, and αα decay has then taken place.

There is more to be learned from nuclear binding energies. The general trend in BE/ABE/A size 12{"BE"/A} {} is fundamental to energy production in stars, and to fusion and fission energy sources on Earth, for example. This is one of the applications of nuclear physics covered in Medical Applications of Nuclear Physics. The abundance of elements on Earth, in stars, and in the universe as a whole is related to the binding energy of nuclei and has implications for the continued expansion of the universe.

Problem-Solving Strategies

Problem-Solving Strategies

For Reaction And Binding Energies and Activity Calculations in Nuclear Physics

  1. Identify exactly what needs to be determined in the problem—identify the unknowns. This will allow you to decide whether the energy of a decay or nuclear reaction is involved, for example, or whether the problem is primarily concerned with activity, rate of decay.
  2. Make a list of what is given or can be inferred from the problem as stated—identify the knowns.
  3. For reaction and binding-energy problems, we use atomic rather than nuclear masses. Since the masses of neutral atoms are used, you must count the number of electrons involved. If these do not balance, such as in β+β+ size 12{β rSup { size 8{+{}} } } {} decay, then an energy adjustment of 0.511 MeV per electron must be made. Also note that atomic masses may not be given in a problem; they can be found in tables.
  4. For problems involving activity, the relationship of activity to half-life, and the number of nuclei given in the equation R=0.693Nt1/2R=0.693Nt1/2 size 12{R= { {1 "." "693"N} over {t rSub { size 8{1/2} } } } } {} can be very useful. Owing to the fact that number of nuclei is involved, you will also need to be familiar with moles and Avogadro’s number.
  5. Perform the desired calculation; keep careful track of plus and minus signs as well as powers of 10.
  6. Check the answer to see if it is reasonable: Does it make sense? Compare your results with worked examples and other information in the text. Heeding the advice in Step 5 will also help you to be certain of your result. You must understand the problem conceptually to be able to determine whether the numerical result is reasonable.

PhET Explorations: Nuclear Fission

Start a chain reaction, or introduce non-radioactive isotopes to prevent one. Control energy production in a nuclear reactor!

This icon links to a P H E T Interactive activity when clicked.
Figure 14.23 Nuclear Fission