Radioactive Decay
Alpha decay: the loss of an α-particle
α-particle: a helium nucleus
Beta decay: the loss of a β-particle
β-particle: a high-energy electron
Positron emission: the loss of a positron
Positron: a particle that has the same mass as, but an opposite charge to, that of an electron
Gamma emission: the loss of a γ-ray
γ-ray: high-energy radiation that almost always accompanies the loss of a nuclear particle:
Electron capture (K-capture): addition of an electron to a proton in the nucleus
The result of this process is that a proton is transformed into a neutron
Nuclear transmutation is a first-order process.
The kinetics of such a process obey this equation:
ln(Nt/N0) = −kt
Nt is the mass, or number of particles at time t.
No is the original.
The half-life of such a process is
0.693/k=t1/2
Comparing the amount of a radioactive nuclide present at a given point in time with the amount normally present, one can find the age of an object.
Alpha decay: the loss of an α-particle
α-particle: a helium nucleus
Beta decay: the loss of a β-particle
β-particle: a high-energy electron
Positron emission: the loss of a positron
Positron: a particle that has the same mass as, but an opposite charge to, that of an electron
Gamma emission: the loss of a γ-ray
γ-ray: high-energy radiation that almost always accompanies the loss of a nuclear particle:
Electron capture (K-capture): addition of an electron to a proton in the nucleus
The result of this process is that a proton is transformed into a neutron
Nuclear transmutation is a first-order process.
The kinetics of such a process obey this equation:
ln(Nt/N0) = −kt
Nt is the mass, or number of particles at time t.
No is the original.
The half-life of such a process is
0.693/k=t1/2
Comparing the amount of a radioactive nuclide present at a given point in time with the amount normally present, one can find the age of an object.