Step 1: Write the expressions for torque and potential energy.
\[
\tau=pE\sin\theta,
\]
\[
U=-pE\cos\theta.
\]
Given,
\[
\tau=0.2\sqrt3\,\mathrm{N\,m},
\]
\[
U=-0.2\,\mathrm{J}.
\]
Step 2: Find the dipole moment.
Squaring and adding,
\[
(pE)^2
=
\tau^2+U^2.
\]
Thus,
\[
pE
=
\sqrt{(0.2\sqrt3)^2+(0.2)^2}
=
\sqrt{0.12+0.04}
=
0.4.
\]
Hence,
\[
p
=
\frac{0.4}{2\times10^5}
=
2\times10^{-6}\,\mathrm{C\,m}.
\]
Step 3: Calculate the charge.
Dipole moment is
\[
p=qd,
\]
where
\[
d=4\,\mathrm{cm}=0.04\,\mathrm{m}.
\]
Therefore,
\[
q
=
\frac{2\times10^{-6}}{0.04}
=
5\times10^{-5}\,\mathrm{C}
=
50\,\mu\mathrm{C}.
\]
Hence,
\[
\boxed{50\,\mu\mathrm{C}}
\]
Therefore,
\[
\boxed{(B)}
\]
is the correct answer.