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 \(\frac{1}{4}\).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)