To solve this problem, we need to determine the time $t$ at which the ratio of the number of nuclei $B$ to nuclei $A$ is $0.3$, given that the half-life of $A$ is $T$. We will use the concept of radioactive decay, where nuclei $A$ decay into $B$.
Radioactive decay follows the equation:
N_A(t) = N_A(0) e^{-\lambda t}
where N_A(t) is the number of nuclei $A$ remaining at time $t$, N_A(0) is the initial number of $A$ nuclei, and \lambda is the decay constant.
The decay constant \lambda is related to the half-life T by:
\lambda = \frac{\log(2)}{T}
The number of nuclei $B$ at time $t$ is the number of $A$ nuclei that have decayed. Therefore:
N_B(t) = N_A(0) - N_A(t)
N_B(t) = N_A(0) - N_A(0) e^{-\lambda t} = N_A(0)(1 - e^{-\lambda t})
We are given that the ratio \frac{N_B(t)}{N_A(t)} = 0.3. Plugging in the expressions, we get:
\frac{N_A(0)(1 - e^{-\lambda t})}{N_A(0)e^{-\lambda t}} = 0.3
\frac{1 - e^{-\lambda t}}{e^{-\lambda t}} = 0.3
1 - e^{-\lambda t} = 0.3 e^{-\lambda t}
e^{-\lambda t} = \frac{1}{1.3}
Taking the natural logarithm on both sides, we have:
-\lambda t = \log\left(\frac{1}{1.3}\right) = -\log(1.3)
\lambda t = \log(1.3)
Substitute the expression for \lambda:
\frac{\log(2)}{T} t = \log(1.3)
Solving for t:
t = T \frac{\log (1.3)}{\log (2)}
Therefore, the correct answer is:
t = T \frac{\log \, (1.3)}{\log \, 2}
The electric potential at the surface of an atomic nucleus \( (z = 50) \) of radius \( 9 \times 10^{-13} \) cm is \(\_\_\_\_\_\_\_ \)\(\times 10^{6} V\).
In a nuclear fission reaction of an isotope of mass \( M \), three similar daughter nuclei of the same mass are formed. The speed of a daughter nuclei in terms of mass defect \( \Delta M \) will be: