To address this issue, the relationship between the decay constant and the quantity of nuclei remaining over time must be understood. Radioactive nuclear decay follows the equation:
\(N(t) = N_0 e^{-\lambda t}\)
where:
Given that the decay constant for nucleus \( n_2 \) is thrice that of nucleus \( n_1 \), it follows that:
\(\lambda_2 = 3\lambda_1\)
The half-life \((T_{1/2})\) of a radioactive sample is linked to its decay constant by the formula:
\(T_{1/2} = \frac{\ln 2}{\lambda}\)
Considering one half-life of nucleus \( n_1 \):
\(T_{1/2,1} = \frac{\ln 2}{\lambda_1}\)
After one half-life, half of the initial nuclei remain:
\(N_1(T_{1/2,1}) = \frac{N_0}{2}\)
For nucleus \( n_2 \), after the same duration:
\(N_2(T_{1/2,1}) = N_0 e^{-\lambda_2 T_{1/2,1}}\)
Substituting \( \lambda_2 = 3\lambda_1 \) and \( T_{1/2,1} = \frac{\ln 2}{\lambda_1} \):
\(N_2(T_{1/2,1}) = N_0 e^{-3\lambda_1 \cdot \frac{\ln 2}{\lambda_1}} = N_0 e^{-3\ln 2} = N_0 \left(\frac{1}{2}\right)^3 = \frac{N_0}{8}\)
The ratio of the number of \( n_2 \) nuclei to \( n_1 \) nuclei after one half-life of \( n_1 \) is thus:
\(\frac{N_2(T_{1/2,1})}{N_1(T_{1/2,1})} = \frac{\frac{N_0}{8}}{\frac{N_0}{2}} = \frac{1}{4}\)
The correct answer is \(\frac{1}{4}\).
The number of undecayed nuclei \( N \) in a sample of radioactive material as a function of time \( t \) is shown in the figure. Which of the following graphs correctly shows the relationship between \( N \) and the activity \( A \)? 