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A radioactive sample decays with a mean life of 20 \mathrm{~ms}. A capacitor of capacitance 100 \mu \mathrm{F} is charged to some potential and then the plates are connected through a resistance R, The resistance \mathrm{R} for which the ratio of the charge on the capacitance to the activity of the radioactive sample remains constant in time is found \mathrm{y} x \, 100 \Omega. Value of \mathrm{y} is

Option: 1

1


Option: 2

2


Option: 3

3


Option: 4

4


Answers (1)

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The activity of radioactive sample of decay constant \lambda at time t is given by

\mathrm{A}=\mathrm{A}_0 \mathrm{e}^{-\lambda t}                 ........(1)

\text { Where } A_0 \text { is initial activity }

The charge on capacitor in series
RC-circuit after time t is

\mathrm{Q}=\mathrm{Q}_0 \mathrm{e}^{-\frac{\mathrm{t}}{\mathrm{RC}}}                    ........(2)

Where Q_0 is initial charge 

Dividing (2) by (1) , we get

\frac{\mathrm{Q}}{\mathrm{A}}=\frac{\mathrm{Q}_0}{\mathrm{~A}_0} \frac{\mathrm{e}^{\mathrm{t} / \mathrm{RC}}}{\mathrm{e}^{-\lambda t}}

\Rightarrow \frac{Q}{A}=\frac{Q_0}{A} e^{\left(\lambda-\frac{1}{R C}\right) t}

Clearly this ratio will be independent of t if

\lambda-\frac{1}{\mathrm{RC}}=0 \Rightarrow \lambda=\frac{1}{\mathrm{RC}} \Rightarrow \mathrm{R}=\frac{1}{\mathrm{C} \lambda}

\text { or as } \lambda=\frac{1}{\tau}

\begin{aligned} & \Rightarrow R=\frac{\tau}{C}=\frac{20 \times 10^{-3} \mathrm{~s}}{100 \times 10^{-6} \mathrm{~F}}=200 \Omega \\ & \Rightarrow y=2 \end{aligned}

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Rishi

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