The potential at a distance $R/2$ from the centre of a conducting sphere of radius $R$ will be

  • A
    $0$
  • B
    $\frac{Q}{8\pi \varepsilon_0 R}$
  • C
    $\frac{Q}{4\pi \varepsilon_0 R}$
  • D
    $\frac{Q}{2\pi \varepsilon_0 R}$

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