Consider radioactive decays \(A \to B\) with half-life \((T_{1/2})_A\), and \(B \to C\) with half-life \((T_{1/2})_B\). At any time t, the number of nuclides of B is given by
\( (N_B)_t = \frac{\lambda_A{\lambda_B - \lambda_A}(N_A)_0 (e^{-\lambda_A t} - e^{-\lambda_B t}) \),
where \((N_A)_0\) is the number of nuclides of A at \(t = 0\). The decay constants of A and B are \(\lambda_A\) and \(\lambda_B\), respectively.
If \((T_{1/2})_B<(T_{1/2})_A\), then the ratio \(\frac{(N_B)_t}{(N_A)_t}\) at time \(t \gg (T_{1/2})_A\) is}
\((N_A)_t\) is the number of nuclides of A at time t