Physics

Physics

Problem

The half-life of an isotope with a very long half-life cannot be measured by observing its activity as a function of time, since the variation in activity over any reasonable time interval would be too small to be observed. Let mm be the mass in grams of a given isotope of long half-life. a. Show that the number of nuclei present in this quantity is N0=mμNAN_0 = \frac{m}{\mu} N_A where μ\mu is the molar mass of the isotope in g mol−1\text{g mol}^{-1} and NAN_A is the Avogadro constant. b. From A=N0λe−λtA = N_0 \lambda e^{-\lambda t} show that the initial activity is A0=mNAμλA_0 = \frac{m N_A}{\mu} \lambda and hence that the half-life can be determined by measuring the initial activity (in Bq) and the mass of the sample (in grams).

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