Electric field at a distance $r$ from an infinitely long uniformly charged straight conductor,having linear charge density $\lambda$ is $E_1$. Another uniformly charged conductor having same linear charge density $\lambda$ is bent into a semicircle of radius $r$. The electric field at its centre is $E_2$. Then

  • A
    $E_2 = \pi r E_1$
  • B
    $E_2 = \frac{E_1}{r}$
  • C
    $E_1 = E_2$
  • D
    $E_1 = \pi r E_2$

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