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The capacity of an isolated sphere is in...

The capacity of an isolated sphere is increased n times when it is enclosed by an earthed concentric sphere. The ratio of their radii is

A

`(n^(2))/(n-1)`

B

`(n)/(n-1)`

C

`(2n)/(n+1)`

D

`(2n+1)/(n+1)`

Text Solution

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The correct Answer is:
To solve the problem, we need to find the ratio of the radii of two concentric spheres, given that the capacitance of an isolated sphere is increased \( n \) times when it is enclosed by an earthed concentric sphere. ### Step-by-Step Solution: 1. **Understand the Capacitance of a Sphere**: The capacitance \( C \) of an isolated sphere of radius \( A \) is given by the formula: \[ C = 4 \pi \epsilon_0 A \] where \( \epsilon_0 \) is the permittivity of free space. 2. **Capacitance of the Concentric Spheres**: When the isolated sphere of radius \( A \) is enclosed by a larger earthed sphere of radius \( B \), the capacitance \( C' \) of the system is given by: \[ C' = \frac{4 \pi \epsilon_0}{\frac{1}{A} - \frac{1}{B}} = \frac{4 \pi \epsilon_0 AB}{B - A} \] 3. **Given Condition**: According to the problem, the capacitance of the isolated sphere is increased \( n \) times when it is enclosed by the earthed sphere. Thus, we can write: \[ C' = n \cdot C \] Substituting the expressions for \( C' \) and \( C \): \[ \frac{4 \pi \epsilon_0 AB}{B - A} = n \cdot (4 \pi \epsilon_0 A) \] 4. **Simplifying the Equation**: We can cancel \( 4 \pi \epsilon_0 \) from both sides: \[ \frac{AB}{B - A} = nA \] 5. **Rearranging the Equation**: Cross-multiplying gives: \[ AB = nA(B - A) \] Expanding the right side: \[ AB = nAB - nA^2 \] Rearranging terms: \[ nA^2 = nAB - AB \] Factoring out \( AB \): \[ nA^2 = AB(n - 1) \] 6. **Finding the Ratio of Radii**: Dividing both sides by \( A \) (assuming \( A \neq 0 \)): \[ nA = B(n - 1) \] Rearranging gives: \[ \frac{B}{A} = \frac{n}{n - 1} \] ### Final Answer: The ratio of the radii \( \frac{B}{A} \) is: \[ \frac{B}{A} = \frac{n}{n - 1} \]
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