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A solid insulating sphere of radius R is...

A solid insulating sphere of radius R is given a charge Q. If at a point inside the sphere the potential is 1.5 times the potential at the surface, this point will be

A

at a distance of `2R//3` from the centre

B

at the centre

C

at a distance of `2R//3` from the surface

D

data insufficient

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The correct Answer is:
To solve the problem, we need to find the point inside a solid insulating sphere of radius \( R \) where the electric potential is 1.5 times the potential at the surface of the sphere. Let's break down the solution step by step. ### Step 1: Understand the potential inside and on the surface of the sphere The potential \( V \) at a distance \( r \) from the center of a uniformly charged solid insulating sphere of radius \( R \) and total charge \( Q \) is given by: \[ V(r) = \frac{kQ}{2R} \left( 3 - \frac{r^2}{R^2} \right) \quad \text{for } r \leq R \] where \( k \) is Coulomb's constant. The potential at the surface of the sphere (when \( r = R \)) is: \[ V(R) = \frac{kQ}{R} \] ### Step 2: Set up the equation based on the given condition According to the problem, the potential at a point inside the sphere is 1.5 times the potential at the surface. Therefore, we can write: \[ V(r) = 1.5 \times V(R) \] Substituting the expression for \( V(R) \): \[ V(r) = 1.5 \times \frac{kQ}{R} \] ### Step 3: Equate the two expressions for potential Now, we can set the two expressions for potential equal to each other: \[ \frac{kQ}{2R} \left( 3 - \frac{r^2}{R^2} \right) = 1.5 \times \frac{kQ}{R} \] ### Step 4: Simplify the equation We can cancel \( kQ \) from both sides (assuming \( kQ \neq 0 \)): \[ \frac{1}{2R} \left( 3 - \frac{r^2}{R^2} \right) = 1.5 \] Multiplying both sides by \( 2R \): \[ 3 - \frac{r^2}{R^2} = 3R \] ### Step 5: Solve for \( r^2 \) Rearranging the equation gives: \[ -\frac{r^2}{R^2} = 3R - 3 \] Multiplying through by -1: \[ \frac{r^2}{R^2} = 3 - 3R \] ### Step 6: Find the value of \( r \) Now, we can express \( r^2 \): \[ r^2 = R^2 (3 - 3R) \] To find \( r \), we take the square root: \[ r = R \sqrt{3 - 3R} \] ### Step 7: Determine the point inside the sphere Since \( R \) is the radius of the sphere, the only valid solution for \( r \) must be less than or equal to \( R \). The only point where the potential is 1.5 times the surface potential occurs at the center of the sphere when \( R = 0 \). ### Conclusion Thus, the point inside the sphere where the potential is 1.5 times the potential at the surface is at the center of the sphere. **Final Answer:** The point will be at the center of the sphere. ---
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