Exponential decay with dice
The classic highschool modelling of radioactive decay requires many dice, and a little patience.
While it is not possible to predict when any given radioactive nuclei will decay; it is possible to predict with a high degree of probability the average rate of decay for a large number of nuclei within a given sample. This is because the rate of decay for each type of radioactive isotope is a constant and is a characteristic or that given isotope. The decay process is then a statistical process. The decay of a radioisotope is a random event. That is, it is the decay of a given nuclei is not dependent on the environment of the nucleus nor its past history. One can then use statistical analysis to determine the probability of the rate of decay; likewise, one can use statistical analysis to determine the probability that a given die will roll a specific number when tossed. For dice, the probability that a specific number will be tossed is based solely on the number of sides the die has. For 6sided dice, there is a 1 in 6 probability (chance) or rolling a 5 (or any of the numbers 16). For example, if one took one hundred 6sided dice and rolled them all at once and removed all of the 5s that were face up, then how many of the 100 dice would one expect to remove?
Since the probability of rolling a 5 is 1 in 6, then multiply 1/6 by 100. The result is 16.6 or since dice come in whole numbers about 16 or 17 dice would be removed. If 17 are removed from the original 100, there would be 83 remaining. One could then predict in the next roll that the number of dice that would land with the 5 face up would be 1/6 (83) or 13.8. Thus the rate of decay is constant and can be used to simulate radioactive decay
Apparatus:
50 dice, dice thrower
Procedure:
 Count 50 dice into the dice thrower and then cast the dice CAREFULLY onto the bench top. This is throw number, t = 1 with dice number N = 50.
 Count and remove any dice showing a ‘6’. Replace the remaining dice back in the thrower.
 Repeat the above until there are less than six dice left.
 Repeat all of the above twice more.
 For each of your throw numbers (t) calculate the average number of dice before the throw (Nav)

Tabulate your results under the headings: Throw number (t); Average number of dice before throw (Nav); ln (Nav)
 The decrease in the number of dice left after each throw is analogous to the decay of unstable nuclei. Each throw number represents the passage of a certain amount of time, for example 1 second. A graph of ‘average dice after throw’ against ‘number of throw’ would look the same as a graph of ‘number of nuclei left’ against ‘time’ such as you should have come across at GCSE. From this graph you should know how to calculate a halflife value.
 Plot a graph of ‘average dice before throw Nav’ against ‘number of throw, t’ and calculate the ‘halflife’ of the dice in terms of throws.

Plot a graph of ‘ln (Nav)’ against ‘number of throw, t’. This graph should be a straight line of negative gradient.
 Measure the gradient of your second graph, it is equal to the NEGATIVE of the decay constant, of the dice.
 Explain why you would expect the decay constant to equal 1/6th.
 See if your halflife value is equal to ln (2) / as would be expected from theory.
 Why would this experiment would give better results if more dice were used?
 What would you expect your values of ‘halflife’ and ‘decay constant’ to be if: (a) dice with ‘5’ as well as ‘6’ were removed. (b) dice with ‘4’, ‘5’ & ‘6’ were removed.