The activity of a sample of a radio- active material is at time $t_1$ and $ A_2$ at time $ t_2$ (where $ t_2 > t _1 $) if T its mean life is then
$A_1 = A_0 e^{-t_1/t}$ $A=A_0^ {e -\lambda t } = A = A_0e^{-t/t}$ $A_0 = {A_1 \over e-t_1/T} \Rightarrow A_0 = {A_1 e^{t_1 /T}} $ $ Now , A_2 = A_0e^{-t_2/T}$ $ =A_1 e^{t_1/T} e^{-t_2/T}$ $ A_2 = A_1 e(t_1 - t_2)/ T$