$A$ charge $Q$ is distributed over a line of length $L$. Another point charge $q$ is placed at a distance $r$ from the centre of the line distribution. Then the force experienced by $q$ is

  • A
    $\frac{qQ}{4\pi \epsilon_0 (r^2 - L^2)}$
  • B
    $\frac{qQ}{4\pi \epsilon_0 (r^2 - (L/2)^2)}$
  • C
    $\frac{qQ}{4\pi \epsilon_0 r^2}$
  • D
    $\frac{qQL}{4\pi \epsilon_0 r^3}$

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