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The half-life of a radioactive sample is...

The half-life of a radioactive sample is `T`. If the activities of the sample at time `t_(1)` and `t_(2)` `(t_(1) lt t_(2))` and `R_(1)` and `R_(2)` respectively, then the number of atoms disintergrated in time `t_(2)-t_(1)` is proportional to

A

`(R_1-R_2)T`

B

`(R_1+R_2)T`

C

`(R_1R_2)/(R_1+R_2)T`

D

`(R_1+R_2)/T`

Text Solution

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The correct Answer is:
To solve the problem, we need to determine the number of atoms disintegrated in the time interval \( t_2 - t_1 \) in terms of the activities \( R_1 \) and \( R_2 \) at times \( t_1 \) and \( t_2 \) respectively. ### Step-by-Step Solution: 1. **Understanding Activity**: The activity \( R \) of a radioactive sample is defined as the rate of disintegration of atoms, which can be expressed as: \[ R = -\frac{dN}{dt} = \lambda N \] where \( \lambda \) is the decay constant and \( N \) is the number of radioactive atoms present. 2. **Establishing Relationships**: At time \( t_1 \): \[ R_1 = \lambda N_1 \] At time \( t_2 \): \[ R_2 = \lambda N_2 \] Here, \( N_1 \) and \( N_2 \) are the number of atoms at times \( t_1 \) and \( t_2 \) respectively. 3. **Finding the Number of Atoms**: From the equations above, we can express \( N_1 \) and \( N_2 \) in terms of the activities: \[ N_1 = \frac{R_1}{\lambda} \] \[ N_2 = \frac{R_2}{\lambda} \] 4. **Calculating Atoms Disintegrated**: The number of atoms disintegrated between \( t_1 \) and \( t_2 \) is given by: \[ \text{Atoms Disintegrated} = N_1 - N_2 = \frac{R_1}{\lambda} - \frac{R_2}{\lambda} = \frac{R_1 - R_2}{\lambda} \] 5. **Substituting for Decay Constant**: The decay constant \( \lambda \) can be related to the half-life \( T \) of the sample using: \[ \lambda = \frac{\ln 2}{T} \] Substituting this into the equation for atoms disintegrated: \[ \text{Atoms Disintegrated} = \frac{R_1 - R_2}{\frac{\ln 2}{T}} = \frac{(R_1 - R_2) T}{\ln 2} \] 6. **Proportionality**: From the final expression, we can see that the number of atoms disintegrated is proportional to: \[ (R_1 - R_2) T \] ### Conclusion: Thus, the number of atoms disintegrated in the time interval \( t_2 - t_1 \) is proportional to \( (R_1 - R_2) T \).
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