Theory of Radioactive decay

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Theory of Radioactive decay

1st consider an analogous model.

In the dice analogy of radioactive decay, the number of dice which decayed per throw (∆N) is given by

                ∆N = N

                ∆ means a small change

                N is the total number of dice at start

The minus sign indicated that ∆N is ever decreasing and the comes from the probability that advice will show a six when thrown.

2nd – Now consider a real example of radioactive decay. In any such example, if k is the change of decay per second then in a time interval ∆t, a fraction k∆t will decay.

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The “k∆t” term here is equivalent to the in the dice analogy.

So in the real radioactive decay, the number of atoms decaying in an interval of time ∆t is given by:

        

                ∆N = -k∆t.N

Rearranging this, we see that,

                Rate of decay = -kN

This rate of decay is going to vary with time, and so in order to find the rate of decay at “an instant”, ∆t must be small so that N will not change much within it.

What are the units of k?

        

Well, if –kN has units ...

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