Analyzing the Setup
Imagine you are holding a tiny charged particle, perfectly still, in a region of space where both an electric field and a magnetic field exist. The special thing about this region is that both fields are pointing in the exact same direction. They are parallel.
When you release the particle from rest, it's like dropping a ball in gravity, but here, the "gravity" is the electric field. The particle has zero initial velocity.
The Master Equation
To understand what happens next, we need to look at the forces that can act on our charged particle. There are two potential forces at play here: the electric force and the magnetic force.
The electric force is straightforward: Fe=qE. It only depends on the charge and the electric field.
The magnetic force is a bit more complex: Fm=q(v×B). It depends on the charge, the magnetic field, and crucially, the velocity of the particle.
The Initial Push
At the exact moment you release the particle (t=0), its velocity v is zero. Because the magnetic force requires velocity to act, it is completely zero at this instant.
However, the electric force doesn't care if the particle is moving or not. It immediately exerts a force Fe=qE on the particle. This force causes the particle to accelerate in the direction of the electric field.
The Magnetic Force Check
As the particle accelerates, it gains velocity. Because the only force acting on it is the electric force, the particle moves exactly along the electric field lines. So, its velocity vector v is parallel to the electric field E.
But wait, the problem stated that the electric and magnetic fields are parallel! This means the velocity v is also parallel to the magnetic field B.
Let's plug this back into our magnetic force equation. The cross product of two parallel vectors is always zero because the angle between them is 0∘, and sin(0∘)=0. Therefore, Fm=qvBsin(0∘)=0.
Final Conclusion
Even though the particle is now moving through a magnetic field, the magnetic force remains zero for the entire journey. The electric force is the only force acting on the particle, continuously accelerating it in the same direction.
Since the force is always along the direction of motion, the particle will never turn or curve. It will simply move in a straight line.