Solution :
Force on a charged particle in the magnetic field is
$$\left| F \right| = q\left| {v \times B} \right|\,\,{\text{or}}\,\,F = qvB\sin \theta $$
when angle between velocity $$v$$ and magnetic induction $$B$$ is $${180^ \circ }$$ or $${0^ \circ },$$ then
$$F = qvB\sin {180^ \circ } = 0\,\,\left[ {{\text{as}}\,\sin {{180}^ \circ }\,{\text{or}}\,\sin {0^ \circ } = 0} \right]$$

So, the charged particle remains unaffected.