Case (i): Along the electric field.
Force on charge: $F = qE$, acts in the direction of motion. Particle accelerates uniformly along a straight line.
Case (ii): Perpendicular to the electric field.
Force $qE$ acts perpendicular to velocity, causing constant acceleration in one direction and uniform motion in the other. Resulting path is a parabola.
Case (iii): Perpendicular to the magnetic field.
Force $F = qvB$ acts perpendicular to both velocity and $B$. This causes uniform circular motion with radius $r = \tfrac{mv}{qB}$.
Case (iv): Along the magnetic field.
Force $F = q(\vec{v} \times \vec{B}) = 0$, since $\vec{v}$ is parallel to $\vec{B}$. Hence the particle moves in a straight line with constant velocity.
Case (v): In crossed electric and magnetic fields ($E \perp B$).
- Electric field provides linear acceleration.
- Magnetic field provides circular motion.
- Resultant path is a helix (spiral).
Step 6: Conclusion.
The nature of path depends on field configuration: linear, parabolic, circular, or helical.