To solve this problem, we need to understand the relationship between the decay constant and the number of nuclei remaining after a certain time period. The decay of a radioactive nucleus is described by the equation:
\(N(t) = N_0 e^{-\lambda t}\)
where:
Given that the decay constant of nucleus \( n_2 \) is 3 times that of nucleus \( n_1 \), we can write:
\(\lambda_2 = 3\lambda_1\)
The half-life \((T_{1/2})\) of a radioactive sample is related to its decay constant by:
\(T_{1/2} = \frac{\ln 2}{\lambda}\)
Since we are considering one half-life of nucleus \( n_1 \), we have:
\(T_{1/2,1} = \frac{\ln 2}{\lambda_1}\)
After one half-life, the number of nuclei remaining is half of the initial number:
\(N_1(T_{1/2,1}) = \frac{N_0}{2}\)
For nucleus \( n_2 \), which has been decaying for the same time period:
\(N_2(T_{1/2,1}) = N_0 e^{-\lambda_2 T_{1/2,1}}\)
Substituting \(\lambda_2 = 3\lambda_1\) and \(T_{1/2,1} = \frac{\ln 2}{\lambda_1}\), we have:
\(N_2(T_{1/2,1}) = N_0 e^{-3\lambda_1 \cdot \frac{\ln 2}{\lambda_1}} = N_0 e^{-3\ln 2} = N_0 \left(\frac{1}{2}\right)^3 = \frac{N_0}{8}\)
Hence, the ratio of the number of nuclei of \( n_2 \) to the number of nuclei of \( n_1 \) after one half-life of \( n_1 \) is:
\(\frac{N_2(T_{1/2,1})}{N_1(T_{1/2,1})} = \frac{\frac{N_0}{8}}{\frac{N_0}{2}} = \frac{1}{4}\)
Therefore, the correct answer is \(\frac{1}{4}\).
Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \[ (\sin x \cos y)(f(2x + 2y) - f(2x - 2y)) = (\cos x \sin y)(f(2x + 2y) + f(2x - 2y)), \] for all \( x, y \in \mathbb{R}. \)
If \( f'(0) = \frac{1}{2} \), then the value of \( 24f''\left( \frac{5\pi}{3} \right) \) is: