Two concentric spherical surfaces \(P_1\) and \(P_2\) enclose charges \(\dfrac{Q}{2}\) and \(4Q\) as shown in the figure. If \(\phi_1\) and \(\phi_2\) are the electric fluxes linked with the surfaces \(P_1\) and \(P_2\) respectively, then
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By Gauss's law,
\[
\phi=\frac{q_{\text{enclosed}}}{\varepsilon_0}.
\]
Electric flux through a closed surface depends only on the total charge enclosed by that surface, not on the radius or exact position of the charge inside.