The nucleus of every atom (except hydrogen) contains one or more
neutrons and one or more protons. The instability of the nuclei of the
heavy atoms is related to the ratio of the number of neutrons to the
number of protons in the nuclei. Radioactive decay is, in fact, a way
of adjusting these ratios. The adjustment can occur in various ways.
The most common is the emission of alpha particles or beta particles.
An alpha particle is identical with the nucleus of a helium atom and has
two neutrons and two protons bundled together. Loss of an alpha
particle from a nucleus lowers the mass number (the total of protons
and neutrons) of the parent nucleus by four and the atomic number (the
number of protons) by two; the number of neutrons also is reduced by
two.
A beta particle is an electron and has a negative electric charge. When
a beta particle is emitted from a nucleus, the nucleus is changed so
that it has one more proton (which has a positive charge) and one less
neutron (which has no charge); in effect, a neutron has changed into a
proton as the nucleus lost a negative charge. Beta decay occurs in
nuclei with a greater proportion of neutrons than is normal for the
number of protons. Since beta emission increases the proportion of
protons, the process raises the atomic number of the parent nucleus by
one and leaves the mass number the same.
Gamma rays are a form of electromagnetic radiation. They are emitted
when a nucleus shifts from one energy state to a lower energy
state—the energy difference emerging as the gamma radiation. Gamma
emission often accompanies alpha or beta emission, but the production
of gamma rays does not itself alter the atomic number nor the mass
number of the parent.
Nuclei also can decay by emission of a positron, which is a positively
charged electron. When this occurs, the new nucleus has one more
neutron and one less proton than its parent; in effect a proton has
become a neutron as the nucleus loses a positive charge. Positrons
usually are emitted by nuclei that have a greater proportion of
protons than is normal for the number of neutrons.
Another process—internal electron conversion—sometimes occurs in
connection with gamma-ray emission, usually in heavy elements when the
gamma-ray energy is low. Instead of being emitted directly, the gamma
ray strikes an orbital electron, knocking the electron out of the
atom; the gamma ray then disappears. Another electron jumps into the
“hole” in the orbit from which the first electron was emitted, and
this jump—from a higher to a lower energy level—results in the
emission of an X ray (which is similar to a gamma ray, but originates
in the electron orbit region of the atom, not in the nucleus).
Public-domain text, read in full here on John Shaqi.
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