The relationship between the mean life \(\tau\) and the half-life \(t_{1/2}\) of a radioactive material is given by:
\[
t_{1/2} = \tau \ln 2
\]
This comes from the fact that the decay constant \(\lambda = \frac{1}{\tau}\) and the half-life is related to the decay constant by:
\[
t_{1/2} = \frac{\ln 2}{\lambda}
\]
Substituting \(\lambda = \frac{1}{\tau}\), we get \(t_{1/2} = \tau \ln 2\).
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