For a hollow spherical shell (conducting), the electric potential inside the shell (i.
e.
, for \( r<R \)) is constant and equal to the potential at the surface.
\[
V_{\text{inside}} = \frac{1}{4\pi \varepsilon_0} \cdot \frac{Q}{R} \quad (\text{constant})
\]
For \( r \geq R \), the shell behaves like a point charge at the center, and potential decreases as:
\[
V_{\text{outside}} = \frac{1}{4\pi \varepsilon_0} \cdot \frac{Q}{r}
\]
Thus, the correct graph is constant from the center to the surface, then falling as \( \frac{1}{r} \).