For a charged metallic sphere, the electric field at a distance \( r \) from the center of the sphere, where \( r > R \), behaves as if the entire charge is concentrated at the center of the sphere. This is a consequence of the spherical symmetry of the charge distribution, and we can apply Coulomb's law to calculate the electric field.
Step 1: Potential on the Surface of the Sphere.
The potential \( V \) at the surface of the sphere is related to the charge \( Q \) on the sphere and the radius \( R \) of the sphere by the formula:
\[
V = \frac{1}{4\pi\epsilon_0} \cdot \frac{Q}{R},
\]
where:
\( Q \) is the total charge on the sphere,
\( R \) is the radius of the sphere,
\( \epsilon_0 \) is the permittivity of free space.
Rearranging the equation for \( Q \), we get:
\[
Q = 4\pi\epsilon_0 \cdot V \cdot R.
\]
Step 2: Electric Field Outside the Sphere.
Now, we need to calculate the electric field \( E \) at a distance \( r \) from the center of the sphere, where \( r > R \). According to Coulomb's law, the electric field at a distance \( r \) from a point charge is given by:
\[
E = \frac{1}{4\pi\epsilon_0} \cdot \frac{Q}{r^2}.
\]
Substituting the expression for \( Q \) from Step 1:
\[
E = \frac{1}{4\pi\epsilon_0} \cdot \frac{4\pi\epsilon_0 \cdot V \cdot R}{r^2}.
\]
Step 3: Simplifying the Expression.
Simplifying the equation:
\[
E = \frac{V \cdot R^2}{r^2}.
\]
Thus, the magnitude of the electric field at a distance \( r \) from the center of the sphere is:
\[
E = \frac{V \cdot R^2}{r^2}.
\]
Therefore, the correct answer is \( \mathbf{(2)} \).