The radioactivity of a sample is $R_1$ at time $T_1$ and $R_2$ at time $T_2.$ If the half-life of the specimen is $T,$ the number of atoms that have disintegrated in time $(T_2 - T_1)$ is proportional to

  • A
    $(R_1T_1 - R_2T_2)$
  • B
    $(R_1 - R_2) T$
  • C
    $(R_1 - R_2)/T$
  • D
    $(R_1 - R_2) (T_1 - T_2)$

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The radioactivity of a sample at time $T_1$ is $R_1$ and at time $T_2$ is $R_2$. If the mean life of the sample is $T$,then the number of nuclei disintegrated in the time interval $(T_2 - T_1)$ is:

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