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A charge Q is distributed over three concentric spherical shells of radii a, b, c (a< b < c) such that their surface charge densities are equal to one another. The total potential at a point at distance r from their common centre, where r < a, would be :

a. \(\begin{array}{l}\frac{Q}{4\pi \epsilon _{0}(a+b+c)}\end{array} \) b. \(\begin{array}{l}\frac{Q(a+b+c)}{4\pi \epsilon _{0}(a^{2}+b^{2}+c^{2})}\end{array} \) c. \(\begin{array}{l}\frac{Q(ab+bc+ca)}{12\pi \epsilon _{0}(abc)}\end{array} \) d. \(\begin{array}{l}\frac{Q(a^{2}+b^{2}+c^{2})}{4\pi \epsilon _{0}(a^{3}+b^{3}+c^{3})}\end{array} \)... View Article