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The first two terms in the semi empirical binding energy formula deal solely with the intenucleon attraction. (a) Calculate the ratio of the second tern to the first term for \(A=20 .\) What does it say about the surface nucleons? (b) Repeat part (a), but for \(A=220\).

Short Answer

Expert verified
The ratio of the second term to the first term is about 7.34 when \(A = 20\) and 9.97 when \(A = 220\). This suggests that as the size of the nucleus (A) increases, the contribution of surface nucleons to the total binding energy becomes less significant compared to the interior nucleons.

Step by step solution

01

Calculate the Ratio for A=20

Firstly, remember that the first term represents volume effects and is directly proportional to nucleon number, while the second term represents surface effects and is proportional to \(A^{2/3}\). To calculate the ratio, use the equation \(R = A/A^{2/3}\). For \(A = 20\), this becomes \(R = 20/20^{2/3} = 20/2.71 = 7.34\). This means that for a small nuclear, the volume term is much larger than the surface term.
02

Calculate the Ratio for A=220

Similarly, for \(A = 220\), calculate the ratio as \(R = 220/220^{2/3}\). This gives \(R = 220/22.07 = 9.97\). Despite the increase in nucleon number, the ratio has not increased significantly.
03

Interpret the Ratios

These ratios suggest that the surface term does not increase as rapidly as the volume term as the nucleon number increases. This indicates that the increase in nuclear size due to the addition of nucleons primarily occurs in the interior of the nucleus, rather than at the surface. It also suggests that surface nucleons contribute less to the total binding energy of an atom compared to the interior nucleons. By comparing the ratios, we see that as a nucleus becomes larger, the contribution of surface nucleons to the total binding energy becomes less significant.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Nuclear Binding Energy
Understanding nuclear binding energy is essential in nuclear physics. It refers to the energy that holds the nucleus together. It's the difference between the mass of the separated nucleons (protons and neutrons) and the mass of the nucleus. This difference is due to the conversion of mass into energy, as described by Einstein's famous equation, \(E=mc^2\).

  • This energy is a measure of the nucleus's stability.
  • A higher nuclear binding energy indicates greater stability.
  • Calculating binding energy helps scientists understand fusion and fission processes, energy release, and nuclear reactions.
Overall, nuclear binding energy is a central concept for explaining why atomic nuclei are stable and how they react under different conditions.
Volume Term
The volume term in the semi-empirical mass formula is a major contributor to the nuclear binding energy. It accounts for the strong nuclear force acting amongst nucleons in the interior of the nucleus.

  • The nuclear force holds protons and neutrons together despite repulsive forces between protons.
  • The volume term is proportional to the number of nucleons \(A\), representing the bulk of nuclear matter.
  • This term assumes that all nucleons contribute equally to binding energy inside a large volume.
This concept helps explain why, as nuclei grow larger, interior nucleons predominantly determine nuclear binding energy.
Surface Term
In contrast to the volume term, the surface term in the semi-empirical mass formula adjusts for nucleons at the surface of the nucleus. It accounts for the reduction in binding energy for surface nucleons compared to those in the interior.

  • Surface nucleons have fewer neighboring nucleons to bond with, reducing their stability contribution.
  • The term is proportional to \(A^{2/3}\), reflecting that surface effects impact smaller nuclei more.
  • Understanding the surface term clarifies why smaller nuclei have relatively larger surface effects than larger ones.
This concept highlights how nuclear shape and size influence overall binding energy and, ultimately, nuclear stability.
Nuclear Physics
Nuclear physics is the study of atomic nuclei and their constituents, including protons and neutrons. This field forms the foundation for understanding nuclear binding energies, reactions, and properties.

  • Key focuses include nuclear structure, stability, decay, and reactions like fission and fusion.
  • It provides insights into the forces that hold the nucleus together and the energy involved in nuclear interactions.
  • Applications are vast, ranging from energy production and medical treatments to understanding cosmological phenomena.
Overall, nuclear physics offers crucial knowledge that informs both theoretical physics and practical applications in technology and medicine.

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Most popular questions from this chapter

Potassium. \(40(Z=19 . N=21)\) is a radioactive isotope that is rare but not unknown in nature. It is particularly interesting in that it lies along the curve of stability yet decays by both \(\beta^{+}\) and \(\beta^{-}\) - that is, in both directions away from the curve of stability. (a) Identify the daughter nuclei for both decays. (b) Many factors governing nuclear stability are discussed in the chapter (e.g., those in the semiempirical binding energy formula, magic numbers, and even numbers). Identify those that would argue only for \(\beta^{-}\) decay. (c) Which factors argue only for \(\beta^{+}\) decay? (d) Which argue for either \(\beta^{-}\) or \(\beta^{+}\) decay?

In both D-D reactions in equation \((11-18)\). two deuterons fuse to produce nwo particles, a nucleus of \(A=3\) and a free nucleon. Mass decreases because the binding energy of the \(A=3\) nucleus is greater than the combined binding cnergies of the two deuterons. The binding energy of haliam- 4 is even greater still. Why can't the deuterons simply fuse into a helium -4 nucleus and nothing else? Why must muluple particles be produced?

Certain nuclei with half-lives between days and a few years are found in nature in small abundances that do not change al all over many, many years. How is this possible? (Hint: Natural uranium and thorium have ren long half- lives.)

Calculate the binding energy per nucleon of carbon-12.

An untrained but perceptive friend exclaims, "They say that nuclear energy can be released by sticking nuclei togethcr and by breaking them apart. That doesn't make sense"" Straighten out your friend's confusion.

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