Question:

The counting rate observed from a radioactive source at $t = 0$ was $1600$ counts $s^{-1}$, and $t = 8 \,s$, it was $100$ counts $s^{-1}$. The counting rate observed as counts $s^{-1}$ at $t = 6$ s will be

Updated On: Jul 2, 2022
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The Correct Option is D

Solution and Explanation

As we know. $\left[\frac{N}{N_{0}}\right]\quad\quad\quad\quad\ldots\left(i\right)$ n = no. of half life N - no. of atoms left $N_{0}$- initial no. of atoms By radioactive decay law. k - disintegration constant $\therefore \frac{\frac{dN}{dt}}{\frac{dN_{0}}{dt}} = \frac{N}{N_{0}}\quad\quad\quad\ldots\left(ii\right)$ From $\left(i\right)$ and $\left(ii\right)$ we get $\frac{\frac{dN}{dt}}{\frac{dN_{0}}{dt}} = \left[\frac{1}{2}\right]^{n}$ or, $\left[\frac{100}{1600}\right] = \left[\frac{1}{2}\right]^{n}\quad \Rightarrow \left[\frac{1}{2}\right]^{4} = \left[\frac{1}{2}\right]^{n}$ $\therefore n = 4$, Therefore, in 8 seconds 4 half life had occurred in which counting rate reduces to 100 counts $s^{-1}$. $\therefore$ Half life, $T_{\frac{1}{2}} = 2\,sec$ In 6 sec, 3 half life will occur $\therefore \left[\frac{\frac{dN}{dt}}{1600}\right] = \left[\frac{1}{2}\right]^{3}$ $\Rightarrow \frac{dN}{dt} = 200$ counts $s^{-1}$
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Concepts Used:

Nuclei

In the year 1911, Rutherford discovered the atomic nucleus along with his associates. It is already known that every atom is manufactured of positive charge and mass in the form of a nucleus that is concentrated at the center of the atom. More than 99.9% of the mass of an atom is located in the nucleus. Additionally, the size of the atom is of the order of 10-10 m and that of the nucleus is of the order of 10-15 m.

Read More: Nuclei

Following are the terms related to nucleus:

  1. Atomic Number
  2. Mass Number
  3. Nuclear Size
  4. Nuclear Density
  5. Atomic Mass Unit