Tokamak plasma heating with intense, pulsed ion beams

• US 4,548,782 A
• Filed: 03/27/1980
• Issued: 10/22/1985
• Est. Priority Date: 03/27/1980
• Status: Expired due to Term

• Current Assignee: the united states of america as represented by the secretary of the navy
• Original Assignee: the united states of america as represented by the secretary of the navy
• Inventors: Winsor, Niels K., Manheimer, Wallace M.
• Primary Examiner(s): CANGIALOSI, SALVATORE A
• Application Number:
  US06/134,717
• Time in Patent Office: 2,035 Days
• Field of Search: 176/3-5, 376/127-130, 376/135, 315/111.71, 315/111.61, 315/111.41
• US Class Current: 376/127
• CPC Class Codes: G21B 1/23 Optical systems, e.g. for irradiating targets, for heating plasma or for plasma diagnostics
• CPC Class Codes: Y02E 30/10 Nuclear fusion reactors

Abstract

An intense, space-charge-neutralized, pulsed ion beam is used to heat a magnetically-confined plasma, such as tokamak plasma, by injecting the ion beam into the plasma along a trajectory that is generally tangential to the confining magnetic field. The intense ion beam is injected into the tokamak before the plasma is fully formed, the remainder of the plasma is formed around the beam, and the beam transfers its energy to the plasma by classical collisions with the electrons and ions of the plasma. Heating of the plasma can be sufficient to produce breakeven or ignition.

Claims

1. Apparatus for heating a plasma, the plasma being confined in an apparatus of the type wherein the plasma is confined in a vacuum chamber by a magnetic field, comprising:

means for producing a space-charge-neutralized, pulsed, ion beam;

means for directing the ion beam into the magnetic field before the plasma is fully formed; and

means for forming the remainder of the plasma around the beam,

the beam transferring its energy to the plasma by classical collisions with the electrons and ions of the plasma.

2. The apparatus recited in claim 1, wherein the ion beam is directed into the magnetic field along a trajectory generally tangential to the lines of force of the magnetic field.

3. The apparatus recited in claim 1, wherein a vacuum region is formed surrounding the plasma;

and the ion frequency of the beam is very much larger than the square of the gyrofrequency of the beam in the magnetic field, thereby producing a polarization electric field in the beam when it enters the magnetic field, the polarization field enabling the beam to propagate across the vacuum region.

4. The apparatus recited in claim 1 wherein the plasma-forming means includes:

fast pulsed valve means for injecting a puff of gas into the vacuum chamber.

5. A method for heating a plasma confined in a magnetic field in a vacuum chamber comprising the steps of:

(a) producing a space-charge-neutralized pulsed ion beam;

(b) injecting the beam into the magnetic field before the plasma is fully formed; and

(c) forming the remainder of the plasma around the beam,

the beam transferring its energy to the plasma by classical collisions with the electrons and ions of the plasma.

6. The method recited in claim 5 wherein step (b) includes:

directing the beam into the magnetic field along a trajectory generally parallel to the lines of force of the magnetic field.

7. The method recited in claim 5 wherein step (c) includes:

injecting a puff of gas into the vacuum chamber.

8. The method recited in claim 5 including the step of:

(d) inactivating external means for driving a current in the plasma subsequent to step (c) so that the entire plasma current is carried by the ion beam.