Atomic nuclei and radioactive decay processes

Atomic nuclei and radioactive decay processes

We are searching data for your request:

Forums and discussions:
Manuals and reference books:
Data from registers:
Wait the end of the search in all databases.
Upon completion, a link will appear to access the found materials.

Nuclear binding energy and mass defect

The binding energy between the nucleons can be calculated if one uses the Einstein relation of the equivalence of mass and energy as a basis:

E.=mc2E = energym = massc = speed of light

The mass for example one Hey4Core would have to be composed of the sum of the masses of two protons and two neutrons:

2mp=21,6726510-24G=3,3453010-24G2mn=21,6726510-24G =3,3453010-24Gm2p+2n=6,6952010-24G

However, very precise measurements of the mass have shown that the mass of the helium nucleus


amounts to. The bulk of the 4So helium core is around 0.0504⋅10-24G less than the sum of the masses of its core building blocks. This mass difference (mass defect) arises from the fact that when protons and neutrons merge to form a nucleus, a small part of their mass is converted into energy. This energy is released in the form of high-energy radiation (γ-quanta) and also occurs in the form of kinetic energy of the relevant nucleus.

If you want to break such a core down into its core building blocks, exactly this energy has to be used again. The energy is therefore called the nuclear binding energy. The mass defect therefore corresponds exactly to the binding energy of the nucleus via the Einstein relationship.

The larger the mass defect in nucleation, the greater its binding energy.

Video: Stable and Unstable Nuclei. Radioactivity. Physics. FuseSchool (August 2022).