In this problem, we are dealing with the radioactive decay activity at two different times, \(t_1\) and \(t_2\), with corresponding activities \(R_1\) and \(R_2\) respectively. We are required to find the relationship between these activities given the decay constant \(\lambda\).
Radioactive decay follows an exponential decay law. The activity \(R\) at any time \(t\) is given by:
\(R = R_0 \text{e}^{-\lambda t}\)
where:
Given that the activity at time \(t_1\) is \(R_1\) and at a later time \(t_2\) it is \(R_2\), we can write:
\(R_1 = R_0 \text{e}^{-\lambda t_1}\)
\(R_2 = R_0 \text{e}^{-\lambda t_2}\)
To find the relationship between \(R_1\) and \(R_2\), divide the first equation by the second:
\(\frac{R_1}{R_2} = \frac{R_0 \text{e}^{-\lambda t_1}}{R_0 \text{e}^{-\lambda t_2}}\)
Simplifying the above equation, we have:
\(\frac{R_1}{R_2} = \text{e}^{-\lambda t_1 + \lambda t_2}\)
\(\frac{R_1}{R_2} = \text{e}^{\lambda (t_2 - t_1)}\)
Therefore, rearranging gives:
\(R_1 = R_2 \times \text{e}^{\lambda (t_2 - t_1)}\)
To match the given format of the options, we can also write this as:
\(R_1 = R_2 \times \text{e}^{-\lambda (t_1 - t_2)}\)
Thus, option \(R_1 = R_2 \text{e}^{-\lambda(t_1-t_2)}\) is correct. This option correctly reflects the decrease in activity due to decay over the time period.
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: