A radioactive nucleus is being produced at a constant rate $\alpha$ per second. Its decay constant is $\lambda $. If $N_0$ are the number of nuclei at time $t = 0$, then maximum number of nuclei possible are

  • A

    $\frac{\alpha }{\lambda }$

  • B

    ${N_0} + \frac{\alpha }{\lambda }$

  • C

    $N_0$

  • D

    $\frac{\lambda }{\alpha } + {N_0}$

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