The equation F = qVBsinθ, where q is the charge, B is the magnetic field, V is the charge’s velocity, and θ is the angle between the velocity vector and the magnetic field vector, provides the force acting on a charge traveling through a magnetic field.
The angle between the velocity vector and the magnetic field vector in this instance is 0° since the electron is traveling along the line of force in magnetic field B. Sinθ = sin(0°) = 0 implies this.
When we enter sinθ = 0 into the formula F = qVBsinθ, we obtain:
F = qVB(0) = 0.
This indicates that there is no force acting on the electron, so choice D is the right one.
The equation F = qVBsinθ, where q is the charge, B is the magnetic field, V is the charge’s velocity, and θ is the angle between the velocity vector and the magnetic field vector, provides the force acting on a charge traveling through a magnetic field.
The angle between the velocity vector and the magnetic field vector in this instance is 0° since the electron is traveling along the line of force in magnetic field B. Sinθ = sin(0°) = 0 implies this.
When we enter sinθ = 0 into the formula F = qVBsinθ, we obtain:
F = qVB(0) = 0.
This indicates that there is no force acting on the electron, so choice D is the right one.