Safety precautions when working with a radioactive source
Limit the time of exposure
Display warning signs so people are aware a radioactive source is in use
Keep sources an arm's length away from your body at all times, and only ever handle the source using long-handled tongs
How to handle a radioactive source safely
1. Use long-handled tongs
2. Remain at least an arm's length away from it at all times
How to store a radioactive source safely
1. Lock it away in a sealed lead-lined container
2. Display a hazard symbol on the container and at the storage location
Inverse square law of radiation
The intensity of radiation is inversely proportional to the square of the distance from the source. As the distance doubles, the intensity quarters.
Geiger Counter or Geiger-Muller Tube
Device used to measure a radioactive count rate
Why is Cobalt-60 a suitable sourcefor this experiment?
Safe for use in schools
Has a half-life of around 5 years, meaning it can be reused for a number of years
The activity is low enough to be safe, but high enough for measurements to be taken easily
Measuring over a longer period of time
Reduces measurement uncertainty
Preliminary recording before bringing radioactive source into lab
Take background radiation count
Accounting for background radiation in experimental data
Subtract background count from counts for each distance to produce corrected counts (C')
Converting from count to count rate
Divide count by length of time over which it was taken to acquire the count rate (mean number of counts per unit time)
Preliminary experiment with source before main experiment
1. Find maximum distance from source at which you can still get a measurable count
2. Take recordings closer to source to determine suitable time period over which to take readings
Graph to confirm inverse square law
Plot 1/√C' against x - should form a straight line with positive gradient
Plotting 1/√C' against x removes any systematic error in the distance measurements
Systematic error in distance measurements
Location of radioactive source within sealed capsule, and precise location of ionisation in GM tube not known to high precision
Obtaining systematic distance error from graph of 1/√C' against x
The straight line will not cross the x-axis at the origin. The difference between x=0m and the point at which the straight line crosses the x-axis will be the systematic error.
An old gamma source may be unsuitable as its activity may have fallen to a level too low to obtain recordable counts over a large enough range of distances