Question 903 of 949
What is the relationship between mass defect and nuclear binding energy in a nucleus?
- The mass defect is directly proportional to the binding energy, as a larger mass defect indicates a more stable nucleus.
- The mass defect is inversely proportional to the binding energy, meaning a larger mass defect results in a less stable nucleus.
- The mass defect has no effect on the binding energy of a nucleus.
- The mass defect is equal to the binding energy, thus they are interchangeable terms.
Correct Answer:
A
Explanation
### Correct Option: A
**Explanation of the Correct Answer:**
The mass defect and nuclear binding energy are closely related concepts in nuclear physics. To understand this relationship, we need to define both terms:
1. **Mass Defect**: This is the difference between the mass of a fully assembled nucleus and the sum of the individual masses of its constituent protons and neutrons (nucleons). When nucleons come together to form a nucleus, some mass is converted into energy, according to Einstein's equation \(E=mc^2\). This lost mass is what we refer to as the mass defect.
2. **Nuclear Binding Energy**: This is the energy required to disassemble a nucleus into its individual protons and neutrons. It is also the energy released when a nucleus is formed from its constituent nucleons. The greater the binding energy, the more stable the nucleus is, as it indicates that more energy would be required to break it apart.
**Relationship**: The mass defect is directly proportional to the binding energy. This means that a larger mass defect corresponds to a larger binding energy. The reasoning behind this is rooted in the conversion of mass into energy. When nucleons bind together, the mass defect represents the mass that has been converted into binding energy. Therefore, if the mass defect is larger, it indicates that more energy has been released during the formation of the nucleus, leading to a more stable configuration.
**Mathematical Representation**: The relationship can be expressed using the formula:
\[
E_b = \Delta m \cdot c^2
\]
where:
- \(E_b\) is the binding energy,
- \(\Delta m\) is the mass defect,
- \(c\) is the speed of light in a vacuum (approximately \(3 \times 10^8 \, \text{m/s}\)).
This equation shows that as the mass defect (\(\Delta m\)) increases, the binding energy (\(E_b\)) also increases, confirming that they are directly proportional.
### Why the Other Options are Incorrect:
- **Option B**: "The mass defect is inversely proportional to the binding energy, meaning a larger mass defect results in a less stable nucleus."
- This option is incorrect because it contradicts the established relationship between mass defect and binding energy. A larger mass defect indicates a more stable nucleus, not a less stable one.
- **Option C**: "The mass defect has no effect on the binding energy of a nucleus."
- This option is also incorrect. The mass defect is fundamentally linked to the binding energy; they are not independent of each other. The mass defect directly influences the amount of energy that binds the nucleus together.
- **Option D**: "The mass defect is equal to the binding energy, thus they are interchangeable terms."
- This option is misleading. While they are related, they are not the same. The mass defect is a measure of mass lost, while binding energy is the energy equivalent of that mass loss. They are related through the equation \(E_b = \Delta m \cdot c^2\), but they are not interchangeable.
### Summary of Key Points:
- The mass defect is the difference between the mass of a nucleus and the sum of its individual nucleons.
- The nuclear binding energy is the energy required to disassemble a nucleus into its nucleons.
- The mass defect is directly proportional to the binding energy; a larger mass defect indicates a more stable nucleus.
- The relationship is mathematically expressed as \(E_b = \Delta m \cdot c^2\), linking mass defect to binding energy.
This understanding is crucial for grasping the stability of atomic nuclei and the principles of nuclear reactions.