A charge is uniformly distributed over a long rod of length . The electric potential at the point lying at a distance from the end (where are collinear) is:
- A\frac{Q}{4\pi\epsilon_0 L} \ln 3
- B\frac{3Q}{4\pi\epsilon_0 L}
- C\frac{Q \ln 2}{4\pi\epsilon_0 L}
- D\frac{Q}{8\pi\epsilon_0 L}
Solution & Step-by-step Explanation

1. Let the charge density be .2. Consider an element at distance from . The rod extends from to .3. Potential .4. .