Just a bit further down the same page, the point is that the velocity selector allows a charged particle with a certain velocity to shoot straight down the finely tuned system between the plates and in the magnetic field unimpeded. Presumably, if it veers off the middle line just a bit, the particle will be "discarded" if you will. Then, a slit at the end of the velocity selector will allow those particles that are of the certain velocity (v=E/B...and you can tune your velocity selectors E and B fields to get that specific velocity) to continue onward (such as in a mass spectrometer where you want to be sure of the initial velocity...stick a velocity selector in front of your mass spectrometer region, like in the next figure).
The net force is only 0 for those particles with v=E/B.