Concept:
For a uniformly charged spherical shell,
\[
\boxed{V=\frac{1}{4\pi\varepsilon_0}\frac{Q}{R}}
\]
at every point inside the shell as well as on its surface.
The total charge on the shell is
\[
\boxed{Q=\sigma(4\pi R^2)}
\]
where
\[
\sigma=\text{Surface charge density},
\]
\[
R=\text{Radius of the shell}.
\]
Since the observation point is inside the shell (\(r\lt R\)), the potential remains constant throughout the interior.
Step 1: Write the given data.
Given,
\[
R=10\,cm=0.1\,m,
\]
\[
\sigma=20\,pC/cm^2.
\]
Convert the surface charge density into SI units.
Since
\[
1\,pC=10^{-12}C,
\]
and
\[
1\,cm^2=10^{-4}m^2,
\]
therefore,
\[
\sigma
=
20\times10^{-12}\times10^{4}
=
2\times10^{-7}C/m^2.
\]
Step 2: Calculate the total charge on the shell.
Using
\[
Q=\sigma(4\pi R^2),
\]
we obtain
\[
Q
=
2\times10^{-7}\times4\pi\times(0.1)^2.
\]
Since
\[
(0.1)^2=0.01,
\]
\[
Q
=
2\times10^{-7}\times4\pi\times0.01
=
8\pi\times10^{-9}C.
\]
Thus,
\[
\boxed{Q=8\pi\times10^{-9}C.}
\]
Step 3: Calculate the electric potential inside the shell.
Using,
\[
V=\frac{1}{4\pi\varepsilon_0}\frac{Q}{R},
\]
where
\[
\frac{1}{4\pi\varepsilon_0}=9\times10^9.
\]
Substituting,
\[
V
=
9\times10^9
\times
\frac{8\pi\times10^{-9}}{0.1}.
\]
Therefore,
\[
V
=
720\pi\,V.
\]
Hence,
\[
\boxed{V=720\pi\,V.}
\]
Thus, the correct answer is
\[
\boxed{\textbf{Option (C)}}.
\]
Important Observation:
Using the standard electrostatic formula,
\[
\boxed{V=720\pi\,V.}
\]
Hence Option (C) is mathematically correct.