The concept of
mass defect is central to understanding nuclear stability and the energy that holds a nucleus together. Simply put, it is the difference in mass between a nucleus and its constituent protons and neutrons when they are separated.
In the context of the Ne-21 nucleus from the exercise, we calculate the mass defect by adding the mass of the individual protons and neutrons and then subtracting the mass of the nucleus itself. This difference represents the 'missing' mass, which has been converted into binding energy to hold the nucleus together, according to Einstein's mass-energy equivalence principle.
Mathematically, we expressed this as:
- Mass of separated constituents (protons and neutrons) - Mass of the nucleus = Mass defect.
- In numbers: 21.168075 amu (total mass of separate nucleons) - 20.98846 amu (mass of the nucleus) = 0.179615 amu (mass defect).
Understanding this mass defect is crucial because it directly relates to the nuclear binding energy, a measure of the nucleus's stability. The greater the mass defect, the higher the binding energy, indicating a more stable nucleus.