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Grade A
The charged radiations (a
and b) interact
with magnetic fields and electric fields. Gamma rays do not.
This can be summed up in the pictures below:
In an electric field:

The alpha particles, being positively charged,
are attracted towards the negative plate. Beta particles are
negative and are attracted to the positive plate.
For a magnetic field:

The charged particles are deflected by the magnetic
field. Gamma rays, not being
charged, are not affected by either an electric or a magnetic field.
When we are doing counts, we need to take the
background count into account. This we do by timing the count
for a period of time, then doing an average, to give an average count
per second.
average count per second = total
count in the time period ÷ time period
If we measure over 60 seconds, we would divide by 60.
Each count occurs when a nucleus disintegrates and radioactive decay is an entirely random event.
Sometimes there are a lot of counts a second, then only a few. So
again we need to time over a period and do an average.
Therefore:
average activity count per second = total average
count per second - average background per second
The activity of a source is measured in becquerels
(Bq) where 1 Bq = 1 count per second.
A typical alpha decay is that of radium to
form radon, a radioactive gas.

Note that:
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The mass number goes down
by 4;
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The atomic number goes
down by 2;
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The alpha particle is a helium
nucleus.
The alpha particle is NOT a helium atom.
Polonium decays by beta decay
to form Astatine, one of the halogens.

Note that:
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The mass number stays the same;
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The atomic number goes up by 1;
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The beta particle is a high speed
electron;
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The curious looking symbol is an
electron antineutrino (you are not expected to know this for
the exam).
The beta particle (electron) comes from the nucleus, NOT the electron
shells.
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