This differs from the previous problem in and the magnetic field is along the z-direction. Thus Bx = By = 0, Bz = B
Assuming as usual the charge of the electron to be - | e |, we write the equation of motion
The motion is confined to the plane z = 0. Eliminating B from the first two equations,
so, as expected, since magnetic forces do not work,
On the other hand, eliminating V, we also get,
The constant is easily evaluated, since v is zero at ρ = a. Thus,