$A$ radio nuclide $A_1$ with decay constant $\lambda_1$ transforms into a radio nuclide $A_2$ with decay constant $\lambda_2$. If at the initial moment the preparation contained only the radio nuclide $A_1$,then the time interval after which the activity of the radio nuclide $A_2$ reaches its maximum value is:

  • A
    $\frac{\ln(\lambda_2/\lambda_1)}{\lambda_2 - \lambda_1}$
  • B
    $\frac{\ln(\lambda_2/\lambda_1)}{\lambda_2 + \lambda_1}$
  • C
    $\ln(\lambda_2 - \lambda_1)$
  • D
    $e^{-(\lambda_1 - \lambda_2)}$

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