US4115191A
Expired / Lapsed
US
⏱️ 0.0 years remaining
Tokamak plasma heating with intense, pulsed, ion beams
Assignee: United States Department of the Navy
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Filing: 1977-06-14
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Granted: 1978-09-19
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Expires: 1997-06-14
Abstract
Abstract An intense, space-charge-neutralized, pulsed ion beam is used to heat a magnetically-confined plasma, such as a tokamak plasma, by injecting the ion beam into the plasma along a trajectory that is generally perpendicular to the confining magnetic field. For proper beam parameters, the ion beam will propagate across the magnetic field in the vacuum region, penetrate the confined plasma, and deposit its energy in the interior of the plasma.
Inventors
- 👤 Edward Ott
- 👤 Wallace M. Manheimer
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-31 19:48
CPC Classifications
H; H05; H05H; H05H1/00; H05H1/02; H05H1/10; H05H1/12; H05H1/22; Y; Y02; Y02E; Y02E30/00; Y02E30/10
Claims Analysis
Total Claims: 5
Claim 1
Independent Claim
179 words
Apparatus for heating a plasma, said plasma being confined in an apparatus of the type wherein said plasma is confined in a vacuum chamber by a magnetic field and a vacuum region is formed surrounding said plasma, which comprises: means for producing a space-charge-neutralized, pulsed, ion beam; and means for directing said ion beam into the magnetic field, said ion beam being formed so that the square of the ion frequency of said beam is very much larger than the square of the gyrofrequency of said beam in the magnetic field, thereby producing a polarization electric field in said beam when it enters the magnetic field, said polarization field enabling said beam to propagate across the vacuum region, the velocity of said beam is greater than the Alfven speed of said beam in the magnetic field so that said beam will penetrate said plasma, and the velocity of said beam is less than 2√2 times the Alfven speed of said beam in the magnetic field so that said beam will deposit its energy in the interior of said plasma.
Claim 2
Dependent Claim
179 words
Apparatus for heating a plasma, said plasma being confined in an apparatus of the type wherein said plasma is confined in a vacuum chamber by a magnetic field and a vacuum region is formed surrounding said plasma, which comprises: means for producing a space-charge-neutralized, pulsed, ion beam; and means for directing said ion beam into the magnetic field, said ion beam being formed so that the square of the ion frequency of said beam is very much larger than the square of the gyrofrequency of said beam in the magnetic field, thereby producing a polarization electric field in said beam when it enters the magnetic field, said polarization field enabling said beam to propagate across the vacuum region, the velocity of said beam is greater than the Alfven speed of said beam in the magnetic field so that said beam will penetrate said plasma, and the velocity of said beam is less than 2√2 times the Alfven speed of said beam in the magnetic field so that said beam will deposit its energy in the interior of said plasma.
Claim 3
Dependent Claim
30 words
The apparatus recited in claim 1, wherein said ion beam is directed into the magnetic field along a trajectory generally perpendicular to the lines of force on the magnetic field.
Claim 4
Independent Claim
156 words
A method for heating a plasma confined in a magnetic field, the magnetic field confining said plasma so that a vacuum region is formed surrounding said plasma, which comprises: producing a space-charge-neutralized, pulsed ion beam; and injecting said beam into the magnetic field, said ion beam being further characterized by the square of the ion frequency of said beam being very much larger than the square of the gyrofrequency of said beam in the magnetic field, thereby producing a polarization electric field in said beam when it enters the magnetic field, said polarization field enabling said beam to propagate across the vacuum region, and the velocity of said beam being greater than the Alfven speed of said beam in the magnetic field and less than 2√2 times the Alfven speed of said beam in the magnetic field, whereby said ion beam will penetrate said plasma and will deposit its energy in the interior of said plasma.
Claim 5
Independent Claim
156 words
A method for heating a plasma confined in a magnetic field, the magnetic field confining said plasma so that a vacuum region is formed surrounding said plasma, which comprises: producing a space-charge-neutralized, pulsed ion beam; and injecting said beam into the magnetic field, said ion beam being further characterized by the square of the ion frequency of said beam being very much larger than the square of the gyrofrequency of said beam in the magnetic field, thereby producing a polarization electric field in said beam when it enters the magnetic field, said polarization field enabling said beam to propagate across the vacuum region, and the velocity of said beam being greater than the Alfven speed of said beam in the magnetic field and less than 2√2 times the Alfven speed of said beam in the magnetic field, whereby said ion beam will penetrate said plasma and will deposit its energy in the interior of said plasma.
References Cited (Backward Citations)
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1981-09-18 | 1982-03-20 | 1982-09-19 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1985-09-18 | 1986-03-20 | 1986-09-19 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1989-09-18 | 1990-03-20 | 1990-09-19 | $7700.00 | Window Closed / Lapsed |