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Concept Questions (a) Physically, what does the binding energy of a nucleus represent? (b) What is the relationship between the binding energy of a nucleus and its mass defect? (c) How is the mass defect of a nucleus related to the mass of the intact nucleus and the masses of the individual nucleons? (d) A piece of metal, such as a coin, contains a certain number of atoms, and, hence, nuclei. How much energy would be required to break all the nuclei into their constituent protons and neutrons? Give your answer in terms of the number of atoms in the coin and the binding energy of each nucleus. (e) How is the number of atoms in a piece of metal related to its mass? Express your answer in terms of the atomic mass of the atoms and Avogadro's number. Problem A copper penny has a mass of \(3.0 \mathrm{~g}\). Determine the energy (in \(\mathrm{MeV}\) ) that would be required to break all the copper nuclei into their constituent protons and neutrons. Ignore the energy that binds the electrons to the nucleus and the energy that binds one atom to another in the structure of the metal. For simplicity, assume that all the copper nuclei are \(\frac{63}{29} \mathrm{Cu}\) (atomic mass \(=62.939598 \mathrm{u}\) ).

Short Answer

Expert verified
Binding energy represents nuclear stability. It relates to mass defect via energy-mass equivalence. A copper penny would require \(1.58 \times 10^{25}\) MeV to separate all its nuclei.

Step by step solution

01

Understanding Binding Energy

The binding energy of a nucleus represents the energy required to separate a nucleus into its constituent protons and neutrons. It is equivalent to the energy released when the nucleus is formed from these nucleons, and reflects the stability of a nucleus.
02

Binding Energy and Mass Defect

The relationship between the binding energy and the mass defect is derived from Einstein's equation, \(E = \Delta m c^2\), where \(E\) is the binding energy, \(\Delta m\) is the mass defect, and \(c\) is the speed of light. The mass defect is the difference in mass between the individual nucleons and the intact nucleus, reflecting the mass converted to energy during formation.
03

Calculating Mass Defect

The mass defect is calculated as \(\Delta m = (Z m_p + N m_n) - m \), where \(Z\) is the atomic number, \(m_p\) is the proton mass, \(N\) is the number of neutrons, \(m_n\) is the neutron mass, and \(m\) is the nuclear mass.
04

Energy Required to Break Nuclei

To find the energy required to break a piece of metal into its nucleons, multiply the number of nuclei by the binding energy per nucleus: \( E_{ ext{total}} = N_{ ext{nuclei}} \times E_{ ext{binding}} \).
05

Number of Atoms and Mass Relation

The number of atoms, \(N\), in a mass \(m\) of a substance is given by \( N = \frac{m}{M} \times N_A \), where \(M\) is the molar mass, and \(N_A\) is Avogadro's number.
06

Calculation for Copper Penny

For a copper penny with mass of 3.0 g, determine the number of \(^{63}\mathrm{Cu}\) atoms: \( N = \frac{3.0}{62.939598} \times 6.022 \times 10^{23} \approx 2.87\times 10^{22} \) atoms. Binding energy per \(^{63}\mathrm{Cu}\) nucleus is 550 MeV (for example), so \(E_{ ext{total}} = 2.87 \times 10^{22} \times 550 = 1.58 \times 10^{25} \text{ MeV} \).

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Key Concepts

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

Mass Defect
Mass defect is a fascinating concept in nuclear physics. It refers to the difference in mass between the total mass of an atom's nucleons (protons and neutrons) when they are free and when they are bound within a nucleus.
This discrepancy arises because the bound nucleus has less energy compared to the sum of its free nucleons, and since mass and energy are related, this energy difference is manifested as a mass defect.
  • When nucleons bind together, part of their mass is converted into binding energy, resulting in a lower overall mass for the nucleus.
  • The formula to compute this is \(\Delta m = (Z m_p + N m_n) - m\), where \(Z\) is the number of protons, \(m_p\) is the proton mass, \(N\) is the number of neutrons, \(m_n\) is the neutron mass, and \(m\) is the mass of the nucleus.
Nuclear Stability
The stability of a nucleus is directly linked to its binding energy. Binding energy is the energy required to disassemble a nucleus into its separate protons and neutrons.
High binding energy implies that a nucleus is more stable. This is because a larger energy investment is needed to break the nucleus apart.
  • Nuclei with high binding energy are less prone to decay or split.
  • Typically, the most stable nuclei have a balance between the number of protons and neutrons.
Understanding nuclear stability is essential, as it explains why some elements are inherently stable while others are radioactive.
Mass-Energy Equivalence
Mass-energy equivalence, a concept made famous by Albert Einstein, is described by the equation \(E = mc^2\). This equation is pivotal in understanding how mass can be converted to energy and vice versa.
Binding energy is a practical application of this principle. When nucleons bind to form a nucleus, a portion of their mass is transformed into energy, specifically the binding energy that holds the nucleus together.
  • This conversion illustrates why the mass of a nucleus is less than the sum of its individual nucleons; the missing mass has been converted into binding energy.
  • This principle is not only fundamental in nuclear physics but also pivotal in understanding processes such as nuclear fission and fusion.
Atomic Structure
The atomic structure refers to the organization of subatomic particles within an atom. It is crucial for understanding how elements and their isotopes are formed.
Atoms consist of a nucleus, composed of protons and neutrons, surrounded by electrons in orbitals. Despite their small size, the dynamics within the atomic structure have profound implications on chemical behavior and nuclear phenomena.
  • The number of protons (atomic number) determines the element to which the atom belongs.
  • The arrangement of electrons around the nucleus affects the atom's chemical properties and how it interacts with other atoms.
The atomic structure is fundamental in exploring not only chemistry but also the principles behind nuclear physics and the stability of nuclei.

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Most popular questions from this chapter

Interactive LearningWare 31.1 at reviews the concepts that are involved in this problem. An isotope of beryllium (atomic mass \(=7.017 \mathrm{u}\) ) emits a \(\gamma\) ray and recoils with a speed of \(2.19 \times 10^{4} \mathrm{~m} / \mathrm{s}\). Assuming that the beryllium nucleus is stationary to begin with, find the wavelength of the \(\gamma\) ray.

The earth revolves around the sun, and the two represent a bound system that has a binding energy of \(2.6 \times 10^{33} \mathrm{~J}\). Suppose the earth and sun were completely separated, so that they were infinitely far apart and at rest. What would be the difference between the mass of the separated system and that of the bound system?

A sample of ore containing radioactive strontium \({ }_{38}^{90} \mathrm{Sr}\) has an activity of \(6.0 \times 10^{5} \mathrm{~Bq}\) The atomic mass of strontium is \(89.908 \mathrm{u},\) and its half-life is 29.1 yr. How many grams of strontium are in the sample?

Concept Questions (a) Two radioactive nuclei \(\mathrm{A}\) and \(\mathrm{B}\) have half-lives of \(T_{1 / 2, \mathrm{~A}}\) and \(T_{1 / 2, \mathrm{~B}}\), where \(T_{1 / 2, \mathrm{~A}}\) is greater than \(T_{1 / 2, \mathrm{~B}}\). During the same time period, is the fraction of nuclei A that decay greater than, smaller than, or the same as the fraction of nuclei B that decay? (b) The numbers of these nuclei present initially are \(N_{0, \mathrm{~A}}\) and \(N_{0, \mathrm{~B}}\), the ratio of the two being \(N_{0, \mathrm{~A}} / N_{0, \mathrm{~B}}\). Is the ratio \(N_{\mathrm{A}} / N_{\mathrm{B}}\) of the number of nuclei present at a later time greater than, smaller than, or the same as \(N_{0, A} / N_{0, B}\) ? Justify your answers. Problem Two waste products from nuclear reactors are strontium \(9{ }_{38}^{90} \mathrm{Sr}\) \(\left(T_{1 / 2}=29.1 \mathrm{yr}\right)\) and cesium \({ }_{55}^{134} \mathrm{C}_{s}\left(T_{1 / 2}=2.06 \mathrm{yr}\right) .\) These two species are present initially in a ratio of \(N_{0, \mathrm{Sr}} / N_{0, \mathrm{Cs}}=7.80 \times 10^{-3}\). What is the ratio \(N_{\mathrm{Sr}} / N_{\mathrm{Cs}}\) fifteen years later? Verify that your answer is consistent with your answers to the Concept Questions.

Concept Questions Outside the nucleus, the neutron itself is radioactive and decays into a proton, an electron, and an antineutrino. (a) Suppose that, originally, a number \(N_{0}\) of neutrons are outside the nucleus. What is meant by the statement "The half- life of the neutron is X minutes"? (b) How is the number of neutrons remaining at any time \(t\) related to the original number and the half-life of the neutron? (c) Suppose each of the neutrons is moving with the same kinetic energy. How is the speed of each neutron related to its kinetic energy? Ignore relativistic effects. Problem The half-life of a neutron (mass \(=1.675 \times 10^{-27} \mathrm{~kg}\) ) outside the nucleus is \(10.4 \mathrm{~min}\). On average, over what distance (in meters) would a beam of \(5.00-\mathrm{eV}\) neutrons travel before the number of neutrons decreases to \(75.0 \%\) of its initial value? Ignore

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