Concept:
Outside a charged conducting sphere, the electric potential depends only on the distance from the centre.
\[
V=\frac{1}{4\pi\varepsilon_0}\frac{Q}{R}
\]
for every point situated at the same radial distance \(R\).
Hence all points on a concentric circle (or spherical surface) are equipotential.
Step 1: Compare the potentials at points \(A\), \(B\) and \(C\).
From the figure,
\[
OA=OB=OC=R.
\]
Therefore,
\[
V_A=V_B=V_C
=
\frac{1}{4\pi\varepsilon_0}\frac{Q}{R}.
\]
Step 2: Calculate work done in moving charge \(q\).
Work done in moving a charge between two points is
\[
W=q(V_i-V_f).
\]
For motion from \(A\) to \(B\),
\[
W_{AB}
=
q(V_A-V_B)
=
0.
\]
Similarly, for motion from \(A\) to \(C\),
\[
W_{AC}
=
q(V_A-V_C)
=
0.
\]
Step 3: Interpret the result.
Since \(A\), \(B\) and \(C\) lie on the same equipotential surface,
\[
\Delta V=0
\]
for both paths.
Hence no work is required in either case.
\[\begin{aligned}
\boxed{W_{AB}=W_{AC}=0}
\end{aligned}\]
Therefore,
\[
\boxed{\text{No work is done in either of the cases.}}
\]
Hence, option \(\mathbf{(D)}\) is correct.