Half Life
Marie Curie thought that the strength of a radioactive source
and therefore the number of particles or gamma rays that it emitted every second did not change
with time but in fact she was wrong. The strength gets weaker as time goes by. Every time the
source emits a particle its activity decreases. There will be fewer radioactive atoms and more
stable ones.
The following graph shows how the activity of a source (in counts per second)
decreases with time.

It's very difficult to
decide when a source has lost ALL of its radioactivity but the time for it to drop to HALF its original
value can be found easily.
The average time taken for the activity of a sample of
radioactive material to drop to HALF its original value is called the
HALF LIFE of the source
(T).
This half-life depends only on the material of the source and different radioactive
isotopes have different half lives.
This means that if we have some
material that has a half life of 20 days then after 20 days it will only be HALF as radioactive as it
was at the start, after another 20 days, i.e 40 days after the start it will only be a quarter as
radioactive, one eight after 60 days and so on.
We can show this in another way by the
following diagram. If we start with a sample of material where all the nuclei are radioactive and
then watch how this changes as time goes by we will see that the number of radioactive nuclei
gets less while the number of non-radioactive nuclei gets greater. The total number of nuclei in
the sample stays the same.
Examples of some common half lives are
shown in the following table:

As the source decays it looses alpha, beta or gamma
radiation and so as time goes by there will be fewer radioactive atoms and more non - radioactive
ones. The
MASS of the
RADIOACTIVE part of the sample gets less. Remember that the total
number of atoms (radioactive and stable) stays the same.
We will see later that
knowledge of the half-lives of radioactive isotopes has been useful in dating rocks and
archaeological specimens. They are also the basis of atomic clocks.

The rate at which a particular radioactive source decays
depends ONLY on the source. It cannot be changed by any physical (e.g. temperature, pressure)
or chemical process.