Steady state compact toroidal plasma production

• US 4,601,871 A
• Filed: 05/17/1983
• Issued: 07/22/1986
• Est. Priority Date: 05/17/1983
• Status: Expired due to Fees

• Current Assignee: United States Department Of Health And Human Services
• Original Assignee: United States Department of Energy
• Inventors: Turner, William C.
• Primary Examiner(s): Kyle, Deborah L.
• Assistant Examiner(s): Wendtland, Richard W.
• Application Number:
  US06/495,386
• Time in Patent Office: 1,162 Days
• Field of Search: 313/231.41, 313/231.51, 313/362.1, 315/111.41, 315/111.61, 315/111.71, 376/107, 376/128, 376/139, 376/143, 376/144, 376/145
• US Class Current: 376/144
• CPC Class Codes: H05H 1/16 using externally-applied electric and magnetic fields
• CPC Class Codes: H05H 1/52 using exploding wires or spark gaps H05H1/26 takes precedence; spark gaps in general H01T
• CPC Class Codes: Y02E 30/10 Nuclear fusion reactors

Abstract

Apparatus and method for maintaining steady state compact toroidal plasmas. A compact toroidal plasma is formed by a magnetized coaxial plasma gun and held in close proximity to the gun electrodes by applied magnetic fields or magnetic fields produced by image currents in conducting walls. Voltage supply means maintains a constant potential across the electrodes producing an increasing magnetic helicity which drives the plasma away from a minimum energy state. The plasma globally relaxes to a new minimum energy state, conserving helicity according to Taylor'"'"'s relaxation hypothesis, and injecting net helicity into the core of the compact toroidal plasma. Controlling the voltage so as to inject net helicity at a predetermined rate based on dissipative processes maintains or increases the compact toroidal plasma in a time averaged steady state mode.

Claims

1. An apparatus for maintaining a field-reversed toroidally shaped plasma in a steady state mode comprising:

at least one magnetized coaxial plasma gun for forming a toroidal plasma said means having cylindrically symmetric solenoidal electrodes for generating a poloidal magnetic field;

means for maintaining the radial equilibrium of said toroidal plasmas after formation, said means being operatively coupled to said plasma gun; and

means for producing magnetic helicity being operatively connected to said electrodes so as to produce increasing magnetic helicity from magnetic flux between said electrodes.

2. An apparatus for maintaining a steady state field-reversed toroidal plasma as recited in claim 1 wherein said means for producing magnetic helicity is a DC electrical power supply electrically connected to said electrodes through switching means.

3. An apparatus for maintaining a steady state toroidal plasma as recited in claim 1 wherein said means for maintaining radial equilibrium is a flux conservor having substantially cylindrical electrically conductive walls producing equilibrium magnetic fields by eddy currents in said conductive walls with the radius predetermined by the dimensions of said plasma gun and said toroidally shaped plasma.

4. The apparatus for maintaining steady state field-reversed toroidal plasma as recited in claim 1 wherein said means for maintaining radial equilibrium is an array of poloidal magnetic field coils.

5. An apparatus for producing steady state field-reversed toroidal plasmas comprising:

at least one magnetized coaxial plasma gun for forming toroidally shaped plasmas having cylindrically symmetric solenoidal electrodes for generating a poloidal magnetic field, electrical input means for said electrodes, gas input means providing particle species for a discharge between said electrodes, and an open annular breech for passage of resulting toroidal plasmas;

means for maintaining the radial equilibrium of said toroidal plasma after formation being operatively coupled to said plasma gun; and

means for producing a constant voltage electrically connected to said electrodes through switching means.

6. An apparatus for producing steady state toroidal plasmas as recited in claim 5 further comprising a coating on the surfaces of said electrodes, said coating capable of having isotopes of hydrogen absorbed thereon.

7. An apparatus for producing steady state toroidal plasma as recited in claim 6 wherein said coating is a metallic liner made of material from the group consisting of tantalum, titanium, vanadium, zirconium or paladium.

8. An apparatus for producing steady state field-reversed toroidal plasma as recited in claim 5 wherein said means for producing a voltage is a regulated DC electrical power supply having;

AC input means;

transformer means having a primary winding connected to said AC input means and a secondary winding;

rectifier means connected to said secondary winding; and

regulation means connected to said rectifier means for adjusting the output voltage.

9. A method for producing steady state field-reversed toroidal plasmas using a magnetized coaxial plasma gun having cylindrically symmetric solenoidal electrodes for generating a poloidal magnetic field, electrical input means for said electrodes, gas input means providing particle species for a discharge between said electrodes, and an open annular breech for passage of a resulting compact toroidal plasma, the method comprising the steps of:

flowing a particle species between said coaxial gun electrodes in sufficient quantity for creating a plasma upon application of predetermined discharge currents;

forming a toroidal plasma by discharging an electrical energy storage means across said electrodes through a particle medium;

confining said toroidal plasma in a radial equilibrium field immediately adjacent to said plasma gun; and

producing an increasing magnetic helicity between said electrodes.

10. The method for producing steady state field-reversed toroidal plasmas as recited in claim 9 wherein said step of producing an increasing magnetic helicity between said electrodes further comprises the step of applying a continuous DC voltage to said electrodes, said voltage maintained at a constant level equal to or greater than the quantity ##EQU13## .

11. The method for producing steady state field-reversed toroidal plasmas as recited in claim 10 wherein the step of applying a continuous voltage to said electrodes further comprises the step of converting AC voltages supplied by conventional utility sources to DC voltages with a regulated DC power supply means.

12. The method for producing steady state field-reversed toroidal plasmas as recited in claim 9 wherein the step of forming an increasing magnetic helicity between said electrodes further comprises the step of applying a constant DC voltage pulse to said electrodes, said voltage equal to or greater than the quantity ##EQU14## said pulse length predetermined by the known relaxation time of the toroidal plasma configuration.

13. The method for producing steady state field-reversed toroidal plasmas as recited in claim 9 further including the step of heating said toroidal plasma with at least one particle beam directed so as to intersect said toroidal plasma.

14. The method for producing steady state field-reversed toroidal plasmas as recited in claim 9 further including the step of heating said toroidal plasma with radio frequency waves directed at said toroidal plasma by at least one transmission antenna.

15. The method for producing steady state field-reversed toroidal plasmas as recited in claim 9 further including the step of introducing deuterium or tritium into said particle species.