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A ring of radius R is charged uniformly ...

A ring of radius R is charged uniformly with a charge `+Q`. The potential at a point on its axis at a distance 'r' from any point on ring will be-

A

`(kQ)/(sqrt(R^(2)+r^(2)))`

B

`(kQ)/(r)`

C

`(kQ)/((r^(2)+R^(2))^(3//2))`

D

`(kQ)/(r^(2))(r^(2)-R^(2))^(1//2)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the electric potential at a point on the axis of a uniformly charged ring, we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Configuration**: - We have a ring of radius \( R \) uniformly charged with a total charge \( +Q \). - We want to find the electric potential at a point \( P \) located on the axis of the ring at a distance \( r \) from the center of the ring. 2. **Identifying the Element of Charge**: - Consider a small element of charge \( dq \) on the ring. The total charge \( Q \) is uniformly distributed along the ring. 3. **Calculating the Potential due to the Charge Element**: - The potential \( dV \) at point \( P \) due to the charge element \( dq \) is given by the formula: \[ dV = \frac{k \, dq}{d} \] where \( k \) is Coulomb's constant and \( d \) is the distance from the charge element \( dq \) to the point \( P \). 4. **Finding the Distance \( d \)**: - The distance \( d \) can be calculated using the Pythagorean theorem: \[ d = \sqrt{R^2 + r^2} \] where \( R \) is the radius of the ring and \( r \) is the distance from the center of the ring to point \( P \). 5. **Integrating to Find Total Potential**: - Since the potential due to each infinitesimal charge \( dq \) is the same at point \( P \) (due to symmetry), we can integrate over the entire ring: \[ V = \int dV = \int \frac{k \, dq}{\sqrt{R^2 + r^2}} \] - The total charge \( Q \) can be expressed as: \[ Q = \int dq \] - Therefore, the total potential \( V \) at point \( P \) becomes: \[ V = \frac{k \, Q}{\sqrt{R^2 + r^2}} \] 6. **Final Result**: - The potential at point \( P \) on the axis of the ring is: \[ V = \frac{kQ}{\sqrt{R^2 + r^2}} \]
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