Charge $q$ is uniformly distributed over a thin half ring of radius $R$. The electric field at the centre of the ring is

  • A
    $\frac{q}{2{\pi ^2}{\varepsilon _0}{R^2}}$
  • B
    $\frac{q}{4{\pi ^2}{\varepsilon _0}{R^2}}$
  • C
    $\frac{q}{4\pi {\varepsilon _0}{R^2}}$
  • D
    $\frac{q}{2\pi {\varepsilon _0}{R^2}}$

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