$A$ particle with charge $Q$ coulomb,tied at the end of an inextensible string of length $R$ metre,revolves in a vertical plane. At the centre of the circular trajectory,there is a fixed charge of magnitude $Q$ coulomb. The mass of the moving charge $M$ is such that $Mg = \frac{Q^2}{4 \pi \epsilon_0 R^2}$. If at the highest position of the particle,the tension of the string just vanishes,the horizontal velocity at the lowest point has to be

  • A
    $0$
  • B
    $2 \sqrt{g R}$
  • C
    $\sqrt{2 g R}$
  • D
    $\sqrt{5 g R}$

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