Well, suppose that the central plasma has a potential equal to the ground because there is a sufficient supply of electrons. The plasma ions are hot, say 30keV. The electrons have 0 keV by assumption when the reach the central plasma. They are heated by the ions by colllision. Now their total energy is greater than the ground potential, so if they escape the cusp they will still have the kinetic energy corresponding to their central temperature left when they get to the wall, at ground potential again. They will hit the wall and be absorbed.Tom Ligon wrote:You seem to have a fundamental misunderstanding, which Dr. Nebel has pointed out repeatedly, of the electron behavior outside the magrid. I have no understanding at all why you persist in thinking the electrons want to go to the walls of a machine with precisely one anode, the magrid. If you object to the emitter being at the same potential as the walls, so that the electrons can, unenthusiastically, go back to the walls, fine, we'll bias the cathode a hundred volts positive of the walls, and that will be that
Or as you say, the emitter could be biased to ensure they impact the wall.