- #1
artis
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- 976
From time to time I think about such ideas among other things.
I know the Penning trap and I see it is a good device for catching small to medium quantities of particles with similar charge. So I thought a little how would one create something similar but for a neutral or quasi neutral plasma.
So instead of having electric field of same polarity electrodes at both vertical ends of the trap as well as a vertical B field let's say we just have a vertical B field where the field lines run either top to bottom or vice versa. The chamber being a cylindrical form the sides of the chamber have electrode pairs that can be switched on and off.Now assume the chamber is already filled with gas mixture which is brought up to plasma state, the vertical B field is already there and then the electrodes are switched on and off in such fashion that one electrode at one side is negative while the electrode at the opposite side of the chamber is positive, when this is done protons would tend to form or at least fly towards the negative sided electrode while electrons to the positive , as the particle would try to realign they would experience the force exerted from the vertical B field as in ordinary Penning traps which would make them curl around the field line and not hit the chamber wall directly. Then before any charge concentration is reached at the wall or before large scale plasma disruption start to take place the electrodes are switched off and the next pair of electrodes are switched on (each time reversing electrode polarity so that the electrons protons have to fly through the middle of the chamber , also the B field is only introduced around the outer radius of the chamber closer to the walls) this way the plasma particles always have to chase the electrodes but while doing so they always curl around the vertical B field preventing their escape into the chamber wall.Presumably the plasma should not also drift into the top or bottom end of the cylindrical chamber because the side electrodes and their E field focuses the particles in the midst on the horizontal axis.Similar configuration could be made linearly with a empty tube and a solenoid forming a solenoid type magnet and electrodes at each end, only here the electrodes would be switched back and forth constantly so that the particles always tend to travel through the tube and the B field guides them. Although I imagine this second topology would have some theoretical problems and limits. How about the first one?
I know the Penning trap and I see it is a good device for catching small to medium quantities of particles with similar charge. So I thought a little how would one create something similar but for a neutral or quasi neutral plasma.
So instead of having electric field of same polarity electrodes at both vertical ends of the trap as well as a vertical B field let's say we just have a vertical B field where the field lines run either top to bottom or vice versa. The chamber being a cylindrical form the sides of the chamber have electrode pairs that can be switched on and off.Now assume the chamber is already filled with gas mixture which is brought up to plasma state, the vertical B field is already there and then the electrodes are switched on and off in such fashion that one electrode at one side is negative while the electrode at the opposite side of the chamber is positive, when this is done protons would tend to form or at least fly towards the negative sided electrode while electrons to the positive , as the particle would try to realign they would experience the force exerted from the vertical B field as in ordinary Penning traps which would make them curl around the field line and not hit the chamber wall directly. Then before any charge concentration is reached at the wall or before large scale plasma disruption start to take place the electrodes are switched off and the next pair of electrodes are switched on (each time reversing electrode polarity so that the electrons protons have to fly through the middle of the chamber , also the B field is only introduced around the outer radius of the chamber closer to the walls) this way the plasma particles always have to chase the electrodes but while doing so they always curl around the vertical B field preventing their escape into the chamber wall.Presumably the plasma should not also drift into the top or bottom end of the cylindrical chamber because the side electrodes and their E field focuses the particles in the midst on the horizontal axis.Similar configuration could be made linearly with a empty tube and a solenoid forming a solenoid type magnet and electrodes at each end, only here the electrodes would be switched back and forth constantly so that the particles always tend to travel through the tube and the B field guides them. Although I imagine this second topology would have some theoretical problems and limits. How about the first one?