The atomic nucleus contains positively charged protons, leading to electromagnetic repulsion between them.
The strong nuclear force holds the nucleus together, overcoming the electromagnetic repulsion, which is crucial for the stability of larger atoms.
This strong nuclear force is responsible for the immense energy released during nuclear reactions, such as fission, which is fundamental to nuclear power and weapons.
Band of Stability
Understanding the band of stability is essential; it relates to the ratio of neutrons to protons in a nucleus.
Stable isotopes are shown in graphs as purple dots; generally, stable nuclei exist for elements with atomic numbers below 80.
For elements above calcium (atomic number 20), more neutrons than protons are needed for stability due to increased electromagnetic repulsion among protons.
The stable ratio can shift; for instance, as the atomic number increases, the required neutron to proton ratio also increases:
Near atomic number 37, the ratio is approximately 1:2 (neutrons:protons).
At around atomic number 80, the ratio is about 1.5:1.
Elements above atomic number 83 are radioactive and unstable. This instability arises because the neutron to proton ratio cannot maintain balance.
Decay Processes
Neutron to proton ratio decides the type of decay a nucleus undergoes.
If a nucleus has too many neutrons, it may experience beta decay, converting a neutron into a proton and thus becoming more stable.
Nuclei with atomic numbers greater than 83 typically undergo alpha emission, losing two protons and two neutrons to achieve stability.
Conservation of Mass in Nuclear Reactions
Unlike chemical reactions, mass is not conserved in nuclear reactions; some mass is converted to energy according to Einstein's equation $E=mc^2$.
This conversion highlights that in nuclear decay processes, a small amount of mass results in a significant energy release.
Half-Life
The half-life ($t_{1/2}$) is the time required for half of the radioactive nuclei in a sample to decay.
For instance, if you start with a 100% sample:
After one half-life, 50% remains;
After two half-lives, 25%;
After three half-lives, 12.5%.
Half-lives can vary greatly:
Carbon-14: $5,730$ years;
Uranium-238: $4.5$ billion years;
Radon-222: $3.8$ days.
Conclusion
Understanding the balance between neutrons and protons is critical in comprehending stability, decay, and the energetic nature of nuclear chemistry.