Mass-Energy Equivalence and Binding Energy
Mass-energy equivalence states that mass and energy are related by E = mc^2. In a nucleus, the mass defect is the difference between the total mass of separated nucleons and the actual nuclear mass, and the corresponding binding energy is the energy needed to separate the nucleus into its nucleons.
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Student-friendly explanation
A stable nucleus has less mass than the sum of its free protons and neutrons. This missing mass is called mass defect and appears as binding energy. Binding energy per nucleon measures average stability per nucleon. The binding energy per nucleon curve rises sharply for light nuclei, reaches a maximum near iron and nickel region, and decreases slowly for heavier nuclei. This graph explains why fusion of light nuclei and fission of heavy nuclei can release energy.
How to write this in exams
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Start with the exact idea
Mass-energy equivalence states that mass and energy are related by E = mc^2. In a nucleus, the mass defect is the difference between the total mass of separated nucleons and the actual nuclear mass, and the corresponding binding energy is the energy needed to separate the nucleus into its nucleons.
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Then show how to use it
Write the given masses in consistent units. Find mass defect by subtracting actual nuclear mass from the sum of separated nucleon masses. Convert mass defect to energy using 931.5 MeV per u or E = delta m c^2. Divide by A if binding energy per nucleon is required. Interpret stability using the graph trend.
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Add one concrete example
If the mass defect of a nucleus is 0.030 u, then binding energy = 0.030 x 931.5 MeV = 27.945 MeV, using 1 u = 931.5 MeV/c^2.
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Avoid this incomplete answer
A frequent wrong answer is to multiply mass defect in atomic mass unit directly by c^2 in SI units without converting u to kilogram. Use either SI units fully or use the MeV shortcut consistently.
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Why is binding energy per nucleon more useful than total binding energy for comparing nuclear stability?
Binding energy per nucleon is more useful because it gives the average binding of each nucleon, so nuclei of different sizes can be compared fairly.
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