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Radius of .2^4 He nucleus is 3 Fermi. Th...

Radius of `._2^4 He` nucleus is `3` Fermi. The radius of `._82^206 Pb` nucleus will be.

A

5 Fermi

B

6 Fermi

C

11.16 Fermi

D

8 Fermi

Text Solution

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The correct Answer is:
To find the radius of the \( _{82}^{206}Pb \) nucleus given that the radius of the \( _{2}^{4}He \) nucleus is 3 Fermi, we can use the formula for the radius of a nucleus: \[ R = R_0 A^{1/3} \] where: - \( R \) is the radius of the nucleus, - \( R_0 \) is a constant (approximately \( 1.2 \, \text{Fermi} \)), - \( A \) is the mass number of the nucleus. ### Step 1: Calculate the radius of the \( _{2}^{4}He \) nucleus. Given: - Mass number \( A \) of \( _{2}^{4}He \) is 4. - Radius \( R \) of \( _{2}^{4}He \) is 3 Fermi. Using the formula: \[ R_{He} = R_0 \cdot 4^{1/3} \] ### Step 2: Set up the equation for the \( _{82}^{206}Pb \) nucleus. For the \( _{82}^{206}Pb \) nucleus: - Mass number \( A \) is 206. Using the same formula: \[ R_{Pb} = R_0 \cdot 206^{1/3} \] ### Step 3: Relate the two radii. From the two equations, we can set up a ratio: \[ \frac{R_{He}}{R_{Pb}} = \frac{R_0 \cdot 4^{1/3}}{R_0 \cdot 206^{1/3}} \] The \( R_0 \) cancels out: \[ \frac{R_{He}}{R_{Pb}} = \frac{4^{1/3}}{206^{1/3}} \] ### Step 4: Substitute the known value of \( R_{He} \). We know \( R_{He} = 3 \, \text{Fermi} \): \[ \frac{3}{R_{Pb}} = \frac{4^{1/3}}{206^{1/3}} \] ### Step 5: Solve for \( R_{Pb} \). Cross-multiplying gives: \[ 3 \cdot 206^{1/3} = R_{Pb} \cdot 4^{1/3} \] Now, solving for \( R_{Pb} \): \[ R_{Pb} = \frac{3 \cdot 206^{1/3}}{4^{1/3}} \] ### Step 6: Calculate \( R_{Pb} \). Calculating the cube roots and substituting: \[ R_{Pb} = 3 \cdot \frac{206^{1/3}}{4^{1/3}} = 3 \cdot \left(\frac{206}{4}\right)^{1/3} \] Calculating \( \frac{206}{4} = 51.5 \): \[ R_{Pb} = 3 \cdot (51.5)^{1/3} \] Using a calculator, \( (51.5)^{1/3} \approx 3.68 \): \[ R_{Pb} \approx 3 \cdot 3.68 \approx 11.16 \, \text{Fermi} \] ### Final Result: The radius of the \( _{82}^{206}Pb \) nucleus is approximately \( 11.16 \, \text{Fermi} \). ---
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