Charges are uniformly spread on the surface of a conducting sphere. The electric field from the center of the sphere in a point outside the sphere varies with distance \( r \) from the center as
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The electric field outside a conducting sphere behaves like that of a point charge, following the inverse square law \( E \propto \frac{1}{r^2} \).
For a conducting sphere, the electric field outside the sphere at a distance \( r \) from the center of the sphere follows the inverse square law:
\[
E = \frac{kQ}{r^2}
\]
where \( k \) is Coulomb's constant, \( Q \) is the total charge on the sphere, and \( r \) is the distance from the center of the sphere.
Therefore, the electric field outside the conducting sphere varies as:
\[
E \propto \frac{1}{r^2}
\]
Thus, the correct answer is:
\[
E \propto \frac{1}{r^2}
\]