If on the concentric hollow spheres of radii $r$ and $R$ $(R > r)$ the charge $Q$ is distributed such that their surface charge densities are the same,then the potential at their common centre is:

  • A
    $\frac{Q(R^2 + r^2)}{4\pi \varepsilon_0(R + r)}$
  • B
    $\frac{QR}{R + r}$
  • C
    Zero
  • D
    $\frac{Q(R + r)}{4\pi \varepsilon_0(R^2 + r^2)}$

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