Physical and mathematical models
Atoms can undergo processes that result in
[[$$E = 2mc^2$$]]
In the case of an electron and a positron, the energy released by this annihilation is of around [[$8\cdot 10^{-14}$]]. So, a gram of electrons and positrons being annihilated equals [[$4\cdot 10^{26}$]] joules of instant energy.
The amount of atoms [[$\Delta N$]] undergoing nuclear reactions in a unit of time [[$\Delta t$]] is proportional to the amount [[$N$]] of atoms that have not reacted yet. Mathematically:
[[$$\frac{\Delta N}{\Delta t} = -\lambda N$$]]
for a constant [[$\lambda$]].
- [[$\alpha$]] radiation, which gives out helium-4 nucleii (which are bundles of two protons and two neutrons)
- [[$\beta^-$]] radiation, which gives out an electron and an antineutrino (the antiparticle of a neutrino)
- [[$\beta^+$]] radiation, which gives out a positron (antiparticle of an electron) and a neutrino
- [[$\gamma$]] radiation, which gives out photons (particles of electromagnetic radiation) of high energy
[[$$E = 2mc^2$$]]
In the case of an electron and a positron, the energy released by this annihilation is of around [[$8\cdot 10^{-14}$]]. So, a gram of electrons and positrons being annihilated equals [[$4\cdot 10^{26}$]] joules of instant energy.
The amount of atoms [[$\Delta N$]] undergoing nuclear reactions in a unit of time [[$\Delta t$]] is proportional to the amount [[$N$]] of atoms that have not reacted yet. Mathematically:
[[$$\frac{\Delta N}{\Delta t} = -\lambda N$$]]
for a constant [[$\lambda$]].