amyy said:
Hi, TSny!
Thank you very much for your reply!
You mentioned that the magnitude of mass excess is the energy required to break the nucleus into individual separated nucleons, and it's often negative. But I also find there are some nuclei whose mass excess is positive, such as M.E. of 3He is 14.931 MeV and it is stable, while that of most "heavy" nuclei is negative. Are the light nuclei exceptional?
I must apologize for thinking that mass excess is the same as mass defect except for sign. As you can see, I now have egg on my face

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Actually, sometimes people do think of them as the same: see
https://en.wikipedia.org/wiki/Nuclear_binding_energy#Mass_defect
But you clearly defined mass excess by the formula you gave and I should have noticed that it was different than mass defect.
Mass defect is the same as binding energy when expressed in the same units. However, mass excess Δ as defined by your formula is something different. Apparently, some tables of nuclides prefer to specify the mass excess rather than the atomic mass itself. Using your formula, it is easy to switch between atomic mass and mass excess using the value of A for the nuclide.
Because the atomic mass of carbon-12 is defined to be exactly 12 atomic mass units, you can check that the mass excess of C-12 is zero: Δ = 0. For other nuclides, Δ can be positive or negative. A negative value generally indicates that the nuclide has a greater binding energy per nucleon than C-12. A positive value of Δ indicates less binding energy per nucleon than C-12.
When you have a nuclear reaction which transforms one or more nuclei into one or more other nuclei, the total A value will be conserved. So, the difference between the initial total Δ and the final total Δ will be the same as the difference in initial and final total masses. This means that when you want to calculate the energy released in a reaction, you can work with mass excess in place of atomic mass. Examples here:
https://people.nscl.msu.edu/~schatz/PHY983_13/Lectures/mass_notes.pdf
I followed your procedure.
The energy needs to be more than the binding energy 8.4819 MeV.E=mn-mp-me=0.782 MeVThe energy released per nucleon is also the binding energy 7.7181 MeVThe energy released in the 2 and 3 step is 8.5001 MeV, which is a little more than the energy 8.4819MeV needed to break apart 3H. If I think right, it is energy favorable. So, the beta decay will happen as long as the process is energy favorable whatever the binding energy (mass excess) is.
Yes, it's energy favorable. But just because it's favorable from an energy point of view doesn't mean that it will actually happen. I think that there could be other factors involved.