Drag the charged particle through the magnetic field. A force F = Bqv acts on it, perpendicular to both its velocity and the field. The green arrow from the particle's centre shows the force — its length grows with the field strength, the charge, and how fast you drag.
A charge q moving with velocity v through a magnetic field B feels a force
F = Bqv (when v is perpendicular to B). Its direction is given by F = qv × B:
always perpendicular to the velocity. Because the force is always sideways to the motion, a free charged
particle travels in a circle — the basis of mass spectrometers, cyclotrons and the aurora. Here the
field points into or out of the screen and you drag the charge in the screen plane, so the force lies in
the plane, at right angles to your drag. Reverse the field or flip the charge sign and the force flips too.