Thermonuclear fusion system

• US 4,246,067 A
• Filed: 08/30/1978
• Issued: 01/20/1981
• Est. Priority Date: 08/30/1978
• Status: Expired due to Term

• Current Assignee: William I. Linlor
• Original Assignee: William I. Linlor
• Inventors: Linlor, William I.
• Primary Examiner(s): Cangialosi, S. A.
• Application Number:
  US05/938,321
• Time in Patent Office: 874 Days
• Field of Search: 176/1, 176/3, 176/4, 176/5, 176/7, 176/9, 176/2
• US Class Current: 376/127
• CPC Class Codes: G21B 3/006 Fusion by impact, e.g. cluster/beam interaction, ion beam collisions, impact on a target
• CPC Class Codes: Y02E 30/10 Nuclear fusion reactors

Abstract

This invention discloses apparatus and methods to produce nuclear fusion utilizing fusible material in the form of high energy ion beams confined in magnetic fields. For example, beams of deuterons and tritons are injected in the same direction relative to the machine axis, but the deuteron velocity is sufficiently greater than the triton velocity so that the deuterons overtake the tritons at a relative velocity which produces a high fusion reaction cross section. The momentum of the deuterons is approximately equal to the momentum of the tritons so that both types of ions follow essentially the same path. Thus, the deuteron and triton beams, together with electrons for space charge neutralization, constitute a "moving-plasma", in which fusion reactions occur. Various alternative magnetic field configurations are described for confinement of the high energy ion beams. Methods are given for the starting and steady-state operation of the invention, based on change-of-charge-state trapping of injected material.

Claims

1. In an apparatus for nuclear fusion of the type having:

a. elongated vacuum chamber means with connecting end portions so as to provide an evacuatable containment volume;

said chamber having an axis of symmetry;

b. vacuum pump means communicating with said vacuum chamber so as to maintain a gas pressure less than 10^-3 torr within the vacuum chamber;

c. means for producing magnetic fields so that said magnetic fields are present substantially throughout said vacuum chamber and are re-entrant on themselves;

an improved particle-injection apparatus comprising;

d. means for injecting fusible energetic particles having a kinetic energy greater than 104 electron volts so as to enter said magnetic fields in the direction approximately parallel to the axis of said vacuum chamber so that said particles will follow a closed path;

e. means for changing the charge state of said fusible particles while within said magnetic fields so that the resulting ions are produced within said magnetic fields to form ion beams;

f. said injection and change-in-charge-state being accomplished for a period of time so that said ion beams attain a density greater than 10¹² particles per cubic centimeter;

g. said ion beams consisting of fusible species such as deuterons and tritons whose velocities are approximately in the same direction and whose speeds differ so as to cause fusion reactions in overtaking collisions between said ion beams, this being stated mathematically;

space="preserve" listing-type="equation">V.sub.D =V.sub.T +V.sub.rel

where V_D represents the velocity of one species of fusible ions, such as deuterons, V_T represents the velocity of another species of fusible ions, such as tritons, and V_rel represents the difference in velocity of said fusible species, such as deuterons and tritons;

h. said ion beams such as deuterons and tritons having approximately equal momentum per unit charge this being stated mathematically;

Q_D ;

electric charge of species D

Q_T ;

electric charge of species T

space="preserve" listing-type="equation">Q.sub.T M.sub.D V.sub.D =M.sub.T V.sub.T Q.sub.D

where M_D and V_D represent, respectively, the mass and the velocity of one species of fusible ions, such as deuterons, and M_T and V_T represent, respectively, the mass and the velocity of another species of fusible ions, such as tritons;

i. means for producing electrons within and in the vicinity of said ion beams so as to substantially neutralize the charge of said ion beams, thereby producing an essentially neutral plasma.

2. The invention of claim 1 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined to be of the "strong-focusing" type having alternating-gradients in successive magnets.

3. The invention of claim 1 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined to be of the "strong-focusing" type in the essentially straight portion of said elongated vacuum chamber, and are of the "cyclotron" type, having north and south magnetic poles, positioned at the connecting end portions of the vacuum chamber.

4. The invention of claim 1 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined to be produced by solenoids, for which the magnetic field vector is parallel to the axis of said vacuum chamber.

5. The invention of claim 1 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined in that the magnetic fields are produced by solenoids, said field-producing windings being distributed on the surface of a "figure-eight" configuration.

6. The invention of claim 1 for producing nuclear fusion reactions modified in that means for producing electric fields are further defined in that the electric fields are of the "strong-focusing" type having alternating-gradient electric fields in successive units.

7. The invention of claim 4 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined in that "cyclotron" type magnet means, having north and south poles, are superimposed on the solenoidal windings, at the connecting end portions of the vacuum chamber.

8. The invention of claim 5 for producing nuclear fusion reactions modified in that means for producing magnetic fields are further defined in that "cyclotron" type magnet means, having north and south poles, are superimposed on the solenoidal windings of the figure-eight configuration, at the connecting end portions of the vacuum chamber.

9. The invention of claim 1 for producing nuclear fusion reactions further defined to include deuterons and tritons as the fusible species.

10. The invention of claim 1 for producing nuclear fusion reactions further defined to include deuterons of approximately 1,500,000 electron-volts energy and tritons of approximately 1,000,000 electron-volts energy, as nominal values of kinetic energy after being trapped in the magnetic field.

11. The invention of claim 1 for producing nuclear fusion reactions further defined to include deuterons of approximately 1,800,000 electrons-volts energy and He³, namely doubly-charged helium ions which have the isotopic mass number of three, of 4,800,000 electron-volts energy, as nominal values of kinetic energy after being trapped in the magnetic field, these kinetic energy values being applicable in the laboratory frame of reference and which satisfy the relation:

space="preserve" listing-type="equation">Q.sub.He M.sub.D V.sub.D =Q.sub.D M.sub.He V.sub.He

where Q_D and Q_He represent, respectively, the ionic charges of a deuteron and a helium nucleus, M_D and V_D represent, respectively the mass and the velocity of a deuteron, M_He and V_He represent, respectively, the mass and the velocity of the doubly-charged helium ions which have the isotopic mass number of three.

12. The invention of claim 1 for producing nuclear fusion reactions further defined to include deuterons of approximately 1,600,000 electron-volts energy, tritons of approximately 1,000,000 electron-volts energy, and He³ doubly-charged ions of approximately 4,800,000 electron-volts energy, all three types of ions having velocities in the same direction and essentially parallel to each other and to the axis of the vacuum chamber.