Mass separator with controlled input
View Patent ↗A device for separating particles according to their respective masses includes a substantially cylindrical wall of inner radius, “R wall ”, that surrounds a chamber and defines a longitudinal axis. A multi-species plasma having relatively cold ions is initiated at a first end of the chamber within a relatively small radius, “r source ”, from the longitudinal axis. A hollow cylinder having an outer radius, “R outer ”, is positioned at the second end of the chamber and centered on the axis. Cross electric and magnetic fields (E×B) are established in the chamber that are configured to send ions of relatively high mass on trajectories having a radial apogee, r apogee , that is greater than the cylinder's outer radius (r>R outer ). After reaching apogee, these ions lose energy and strike the cylinder where they are collected. Low mass ions are placed on small radius helical trajectories and pass through the hollow cylinder.
1. A device for separating a multi-constituent material into constituents, said device comprising:
a cylindrical wall having a first end, a second end and an inner radius, R wall , said wall surrounding a chamber and defining a longitudinal axis;
means at said first end of said wall for converting the multi-constituent material into a multi-species plasma in said chamber within a radius, r source , from said longitudinal axis to create cold ions of relatively low mass to charge ratio, M 1 , and cold ions of relatively high mass to charge ratio, M 2 ;
a collector shaped as a hollow cylinder having outer radius R outer , said collector centered on said longitudinal axis and positioned at said second end of said wall;
means for establishing crossed electric and magnetic fields (E×B) in said chamber to define a cutoff mass M C , relative to a radial distance, a, from said axis, with M 1 <M 2 ≦M C and a<R wall ; and
means for controlling E×B to place said ions of relatively high mass to charge ratio, M 2 , on trajectories having a radial apogee, r apogee , into said collector with r apogee >R outer , and to place said ions of relatively low mass to charge ratio, M 1 , on trajectories through said hollow collector.
2. A separator as recited in claim 1 wherein said controlling means is configured to place said ions of relatively high mass to charge ratio, M 2 , on trajectories having a radial apogee, r apogee , greater than the distance, a (r apogee >a).
3. A separator as recited in claim 1 wherein said electric field E is oriented radially with a positive potential (V ctr ) on said longitudinal axis and a substantially zero potential at said radial distance, a, from said longitudinal axis.
4. A separator as recited in claim 1 wherein said controlling means is configured to place said ions of relatively low mass to charge ratio, M 1 , on helical trajectories of diameter D low mass , and said collector has an inner radius R inner , with R inner >D low mass +r source .
5. A separator as recited in claim 1 wherein said establishing means comprises a plurality of ring shaped electrodes that are concentrically arranged about said axis and positioned at a said end of said wall to create said electric field (E) in said chamber.
6. A separator as recited in claim 1 wherein said establishing means comprises at least one coil mounted on said wall to create said magnetic field (B) in said chamber.
7. A device for separating a multi-constituent material into constituents, said device comprising:
a cylindrical wall having an inner radius, R wall , said wall surrounding a chamber and defining a longitudinal axis;
means for converting the multi-constituent material into a multi-species plasma in said chamber within a radius, r source , from said longitudinal axis to create ions of relatively low mass to charge ratio, M 1 , and ions of relatively high mass to charge ratio, M 2 ;
a collector shaped as a hollow cylinder having outer radius R outer , said collector centered on said longitudinal axis and positioned at said second end of said wall;
means for establishing a radial electric field (Er) and an axially aligned magnetic field (B z ) in said chamber to create a plasma region of radius, a, from said axis, with a<R wall ; and
means for controlling said electric field (E r ) and said magnetic field (B z ) to place said ions of relatively high mass to charge ratio, M 2 , on trajectories into said collector, and to place said ions of relatively low mass to charge ratio, M 1 , on trajectories through said hollow collector.
8. A separator as recited in claim 7 wherein said controlling means establishes a cutoff mass, M C , relative to a radial distance, a, from said axis in accordance with the equation:
M C =zea 2 ( B z ) 2 /8 V ctr
where “ze” is the ion charge.
9. A separator as recited in claim 8 wherein said controlling means establishes a cutoff mass, M C , with M 1 <M 2 ≦M C .
10. A separator as recited in claim 7 wherein said cylindrical wall has a first end and a second end, said converting means is positioned at said first end of said wall, and said collector is positioned at said second end of said wall.
11. A separator as recited in claim 7 wherein said radius, r source , is sized to create a multi-species plasma having cold ions.
12. A separator as recited in claim 7 wherein said controlling means is configured to place said ions of relatively high mass to charge ratio, M 2 , on trajectories having a radial apogee, r apogee , with r apogee >Router.
13. A separator as recited in claim 7 wherein said electric field, E r , is established with a positive potential (V ctr ) on said longitudinal axis and a substantially zero potential at said distance, a, from said longitudinal axis.
14. A separator as recited in claim 7 wherein said converting means is configured to generate a plasma having a collisional density, n c , in said plasma region.
15. A separator as recited in claim 7 wherein said converting means is configured to generate a plasma having a collision-less density in said plasma region.
16. A method for separating a multi-constituent material into constituents, said method comprising the steps of:
providing a cylindrical wall having inner radius, R wall , said wall surrounding a chamber and defining a longitudinal axis;
converting the multi-constituent material into a multi-species plasma in said chamber within a radius, r source , from said longitudinal axis to create cold ions of relatively low mass to charge ratio, M 1 , and cold ions of relatively high mass to charge ratio, M 2 ;
centering a hollow cylinder having an outer radius, R outer , on said longitudinal axis;
establishing crossed electric and magnetic fields (E×B) in said chamber to define a cutoff mass, M C , relative to a radial distance, a, from said axis, with M 1 <M 2 ≦M C and a<R wall ; and
controlling E×B to place said ions of relatively high mass to charge ratio, M 2 , on trajectories having a radial apogee, r apogee , into said cylinder with r apogee >R outer , and to place said ions of relatively low mass to charge ratio, M 1 , on trajectories through said hollow cylinder.
17. A method as recited in claim 16 wherein said controlling step places said ions of relatively high mass to charge ratio, M 2 , on trajectories having a radial apogee, r apogee , greater than the radial distance, a (r apogee >a).
18. A method as recited in claim 16 wherein said electric field, E, is oriented radially with a positive potential (V ctr ) on said longitudinal axis and a substantially zero potential at said distance, a, from said longitudinal axis.
19. A method as recited in claim 16 wherein said controlling step places said ions of relatively low mass to charge ratio, M 1 , on helical trajectories of diameter D low mass , and said collector has an inner radius R inner , with R inner >D low mass +r source .
20. A method as recited in claim 16 wherein said establishing step is accomplished with a plurality of ring shaped electrodes that are concentrically arranged about said axis and positioned at a said end of said wall to create said electric field (E) in said chamber.