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Half-life of a radioactive substance A i...

Half-life of a radioactive substance `A` is two times the half-life of another radioactive substance `B`. Initially, the number of `A` and `B` are `N_(A)` and `N_(B)`, respectively . After three half-lives of `A`, number of nuclei of both are equal. Then, the ratio `N_(A)//N_(B)` is .

A

`1//4`

B

`1//8`

C

`1//3`

D

`1//6`

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The correct Answer is:
To solve the problem, we need to analyze the decay of two radioactive substances A and B based on their half-lives and the initial quantities. ### Step-by-Step Solution: 1. **Define the Half-Lives:** Let the half-life of substance B be \( t_{1/2} \). Then, the half-life of substance A is \( 2t_{1/2} \). 2. **Determine the Number of Half-Lives:** After 3 half-lives of substance A, the number of half-lives that have passed for substance B will be: \[ \text{Half-lives of B} = \frac{3 \text{ (half-lives of A)}}{2} = 1.5 \text{ half-lives of B} \] 3. **Calculate Remaining Nuclei of A:** The remaining quantity of substance A after 3 half-lives is given by the formula: \[ N_A = N_{A0} \left(\frac{1}{2}\right)^3 = N_{A0} \cdot \frac{1}{8} \] where \( N_{A0} \) is the initial quantity of substance A. 4. **Calculate Remaining Nuclei of B:** The remaining quantity of substance B after 1.5 half-lives is: \[ N_B = N_{B0} \left(\frac{1}{2}\right)^{1.5} = N_{B0} \cdot \frac{1}{\sqrt{2}} \cdot \frac{1}{2} = N_{B0} \cdot \frac{1}{2\sqrt{2}} \] where \( N_{B0} \) is the initial quantity of substance B. 5. **Set the Remaining Quantities Equal:** According to the problem, after 3 half-lives of A, the number of nuclei of both substances is equal: \[ N_{A0} \cdot \frac{1}{8} = N_{B0} \cdot \frac{1}{2\sqrt{2}} \] 6. **Rearranging the Equation:** Rearranging gives: \[ \frac{N_{A0}}{N_{B0}} = \frac{1}{8} \cdot \frac{2\sqrt{2}}{1} = \frac{2\sqrt{2}}{8} = \frac{\sqrt{2}}{4} \] 7. **Final Ratio:** Therefore, the ratio \( \frac{N_A}{N_B} \) is: \[ \frac{N_A}{N_B} = \frac{1}{8} \] ### Final Answer: The ratio \( \frac{N_A}{N_B} \) is \( \frac{1}{8} \). ---
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