Concept:
The magnetic force acting on a charged particle moving in a magnetic field is given by
\[
F=qvB\sin\theta,
\]
where
\[
q=\text{charge},
\qquad
v=\text{velocity},
\qquad
B=\text{magnetic field},
\]
and \(\theta\) is the angle between \(\vec v\) and \(\vec B\).
Step 1: Identify the angle between velocity and magnetic field.
The particle moves parallel to the magnetic field.
Therefore,
\[
\theta=0^\circ.
\]
Step 2: Substitute into the magnetic force equation.
\[
F=qvB\sin0^\circ.
\]
Since
\[
\sin0^\circ=0,
\]
\[
F=0.
\]
Step 3: State the result.
No magnetic force acts on a charged particle moving parallel (or antiparallel) to the magnetic field.
\[
\boxed{F=0}
\]
\[
\boxed{\text{Answer = (D)}}
\]