US2826708A - Plasma generator - Google Patents

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US2826708A
US2826708A US512904A US51290455A US2826708A US 2826708 A US2826708 A US 2826708A US 512904 A US512904 A US 512904A US 51290455 A US51290455 A US 51290455A US 2826708 A US2826708 A US 2826708A
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plasma
orifice
chamber
gas
wave guide
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Jr John S Foster
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J27/00Ion beam tubes
    • H01J27/02Ion sources; Ion guns
    • H01J27/16Ion sources; Ion guns using high-frequency excitation, e.g. microwave excitation
    • H01J27/18Ion sources; Ion guns using high-frequency excitation, e.g. microwave excitation with an applied axial magnetic field
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10TECHNICAL SUBJECTS COVERED BY FORMER USPC
    • Y10STECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y10S164/00Metal founding
    • Y10S164/04Dental

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Description

v Marchll, 1958 J. s. FOSTER, JR
PLASMA GENERATOR Filed June 2, 1955 zOEbmm INVENTOR. I JOHN S. FOSTER, JR.
BY fiMd 0 AZ'TORNEY.
. ciency is low.
United States atentO PLASMA GENERATOR John- S. Foster, Jr., Livermore, caurl, assignor to-the' United States of America as represented by the United StatesAtomic Energy Commission Application June 2, 1955, Serial No; 512,904 8 Claims. (c1. 3.13:7
Th-is .Sinvention relates to apparatus fonprodiicing ioniz'ed gas. and, more specifically, to. a generator for prowise.
'In conventional; practice the-plasmais usually. accomlision processesofthe. neutral. gas particles and other attendant phenomenon seriously alter the behavior of lthe plasma and may, render suchawplasmaunfit for varioususes. Power requirements irnconventional methods-of plasma production are high andplasma production efli- In conventionall-practice a plasma-may be generatedby electrombombardment of. gas molecules as in an arc discharge. However, ,an electrically neutral ionized gasdischarge has been very difiicult to. obtain.
The device of the present invention providesanuncontamitiatedpalsma notassociated Wuhan electron beam and accomplishnes this result-byinducting ionization. of gas particles in a restricted region and: selectively extracting'the plasma particles through anorifice oflimited size. Since the plasmais selectively extracted, contaminationby, neutral particles is largely eliminated and there is 'no association with an electron beam. The selective extraction is effected'by utilizing an axially symmetric magnetiofield acting, in cooperation with a pressure. differential established through .said orifice whereby the probability of a plasma particle escapingthrough. orificef is h'igh'compared tothat .of .a neutral particle. High" ionization efii'cie'ncy, and maximum power transfer is" ohtainedlby utilizing very high radio frequency generatin'gi'means'efilciently coupled toa plasma. generation chamber by establishing and'maintaining certain critical relationships between the electron plasma frequency, cyclotron frequency of the electrons in the generating chamber, and the operating frequency of the radio fre quency energizing source.
It is therefore an object of the present inventionato provide methods and apparatus for generating a plasma.
Another object of the invention is. to: provide a-generator capable of producing a plasma'uncontaminatedby an electron beam or neutral particles. I
An additional objectlof the-inventionlis toprovid -a plasma generator wherein radio frequencyjenergy: is :employed in the production ofions of a plasma.
Atfurther object of:the:invention. is 'to..provide a generator consuming'minimum-powerin the productionof aplasmaa.
A. stillfurther object .of-the. invention is;.to provide-a plasmagenerator utilizing: an axially symmetric mag- .uetic field actingin cooperation with a pressure difieren-= panie'd'by, antenergetic electron..beam,.and the plasma is highlyflcontaminatedwith neutral gas particles; Colr 2,826,708 Patented Mar. 11, 1958 lie tial'to selectively extr'act'and focus a plasma through an orifice.
The invention, both as to its organization and method of' operation, together with further objects and advantages thereof,lwill best be understood by reference to the followingn'specification taken in conjunction with the accompanyingdrawing, of which:
, Figure 1 is a longitudinalcross sectional view of a preferred embodiment. of'th'e invention; and
Figure 21is'a cross section taken along plane 2-201? Figure-.1.
The plasma generator of the invention is considered suitable. for providing a plasma to be' utilized in a variety of devices characteristically similar in that aplasma, ii e.,-ionized gas,.is employed" therein for sundry purposes. Electrically neutral'plasmas areof interest in the thermonuclear. fields and for experimental purposes;
'pla'sm'a' generator ofthe invention will include an evacuated system into which the plasma is discharged and utilized for diverse experimental purposes.
In'brief, therefore," the plasma generator of the invention' includes means providing anevacuated system in which thereis contained a region; wherein the plasma is to be'utilizedand also a plasma generation chamber having an orificecommunicating with the evacuated sys tem: In this chamberthere is produced animpure plasma contaminated by neutral molecules; For producing said impure plasma there is provided meansfor: introducing a suitable gas to the plasma generation'chamberand thereby establishing a gas pressure difierentialacross said orifice, means for establishing an axially symmetric magnetic fieldnormal-to said orifice, and very high radio frequency generating means-adapted to energize'the' plasma generationchamber-causingionizationof the gasithereinz The along a a path most" favorable for extraction through the orifice; Theextractionof an electrically neutral'uncontaminatedplasma'is accomplished by the focusing action Of-"th e magnetic field cooperating with the'pressure differential establishedacrossthe orifice, as will be more fully disclosed hereinafter: I
More particularly, referring to the accompanying drawing,- the means providing an evacuated system may comprisea'n elongated evacuated cylindricalhousing 11 coupled as by a' conduit tube'12' to'a conventional vacuum pump (not shown); Conveniently, such a housing 11 is-constructed of a 'tubular-section 13 flanged at the extremities forthe' attachment of end cover plates 14 and-16=a's:-bymeans'of flange bolts'17 and 18. Annular vacuum sealing elements '19 and 21-are disposed between the end plates and the flangedextremities of the housing 11 m provide. a vacuum sealth'erebetween. The housing'll'should be constructed of material-perviousto'a magnetic field as will. be apparent from the context'of the specification.
lt will' be'noted here, in the event the plasma generator is used in an apparatus such as anaccelerator or the like, thatthehousing'll may be eliminated and an evacuated regionof" such apparatus may provide the hercinbeforementioned means providing an evacuated system. It will'also'b'e appreciated that the plate 16 located'at theiorwardjextremity'of'the housing 1Imay be eliminated to enable'the housing to be secured directly to such apparatus when" the plasma generator is used therewith. For particular applications of the invention 3 a other means providing an evacuated system will be obvious.
To provide a most convenient and simplified constructionathe plasma generation chamber-may be constructed as an integral extension portion of a tubular wave guide 22 whereby the wave guide is made to serve the multiple purposes of providing structural portions of the said chamber and means for coupling the ionization energy source thereto. More specifically, the wave guide 22 is provided with a terminal flange 23 for the attachment of a cup-shaped terminal chamber member 24 having a tubular wall portion 26 of size and shape similar to said wave guide, an end face 27, and provided after. A D. C. power supply (not shown) is provided with a flange 28 attachable as by means of bolts 29. to
the terminal flange 23 of the wave. guide "22. The periphery of a gas tight partition 31 formed of electrically non-conductor'material is disposed between said flanges 23 and 28 so as to separate the plasma generation chamber proper 24 from the remainder of the wave guide 22, and a sealing element 32 may be disposed outwardly therefrombetween the flanges to provide a more positive vacuum seal.
The end face 27 of the chamber member 24 is centrally apertured to receive an exit tube 33 provdiing an orifice 34 axially aligned with said wave guide 22. Several structural arrangementse may be employed whereby said orifice is made to communicate with the interior of said housing 11. .For structural convenience it is preferred that the wave guide be disposed so as .to pierce or be supported in vacuum tight fashion by one of said cover plates, e. g., plate 14, whereby the wave guide 22 and orifice 34 are in approximate axial alignment with the housing 11.
within an aperture 36 provided in said plate 14 and extending within the housing 11; however, if desired the plasma chamber 24 may be terminated at the plate 14 and with only the tube 33 piercing said plate.
For the purposes of the invention, the wave guide 22 is constructed and proportioned in accordance with conventional practice with regards to tubular transmission lines. While a rectangular guide is shown other tubular guidesmay also be employed. However, for reasons apparent hereinafter the material employed while being necessarily an electrical conductor must also be pervious to a magnetic field, i. e., a non-magnetic electrical conductor is employed in constructing the wave guide and plasma chamber. Also, to minimize heating of the partition -31 the partition is disposed at a minimumcurrent node in the wave guide '22, i. e., the longitudinal length of the plasma generation chamber 24 is preferably made a half-wave length or multiple thereof.
The hereinbefore mentioned means for introducing gas tothe plasma generation chamber may comprise a conduit=37 communicating with an external gas supply 38 andterminating in the plasma generation chamber 24 whereby a pressure differential is established across the orifice 34 by introducing gas therethrough. Gaseous material such as hydrogen, hydrogen isotopes or any other desired gaseous material may be employed, as required for the desired purpose. The conduit 37 as shown in Figure 1 transpierces the plate 14 in gas tight fashion ical structure.
The means for establishing an axially symmetric magnetic field normal to said orifice may comprise a solenoid 43 disposed coaxially about the housing 11 and extending along the longitudinal axis thereof a distance suflicient to provide an axially symmetric magnetic field in both the plasma generation chamber 24 and tthe evacuated region of the housing 11. Specific boundaries of the magnetic field will become more apparent herein- For the most compact arrangement the wave guide 22 is disposed in vacuum tight relation to energize the solenoid 43.
Very high radio frequency energy required to energize said plasma generation chamber can be supplied by various conventional means and may comprise a continuous wave magnetron oscillator 44 coupled to the wave guide 22 as through a matching wave guide section 46. It will be appreciated that any appropriate electrical oscillatory apparatus operating in the microwave region may also be employed such as klystrons and the like. The electromagnetic waves propogating within the wave guide 22 energize the free electrons in the plasma generation chamber 23. Stray electrons always exist in such a system and it is well known in the art that an energetic electron moving in a magnetic field will follow a helical path, the axis of which lies perpendicular to the direction of rotation. Thus the energized electronswill describe a roughly tight helical path and produce ionizati-onas they collide with the gas molecules and a plasma will be thereby formed in the plasma generation chamber 24. V Moreover, the ionized gas molecules being positively ionized will describe generally similar paths, with opposite direction of rotation to the electrons and will form with the electrons an electrical neutral plasma in the chamber. A v f To begin operation of the plasma generator of the invention, the housing 11 is continuously evacuated by said vacuum pump whereby continuous evacuation of the plasmageneration chamber also is efiected. Gas such as deuterium, tritium, and the like from which the plasma is to be generated is then continuously introduced into the generation chamber 24 from the gas supply 33 and at a rate correlated with the ratio of evacuation to establish the desired operating pressure in said chamber and to establish and maintain a gas pressure differential across the orifice 34. f Actuation of the radio frequency energizing means 44 then supplies radio frequency energy to the wave guide 22 wherein the electromagnetic waves propagate to the plasma generation chamber 24. Electrons present therein are caused to accelerate in the aforesaid helical paths by the interaction of electric fields produced by said radio frequency energy and the constraint of said axially magnetic fields producing copious ionization of the gas molecules thereby forming an impure plasma, i. e., neutral atom contaminated electrically neutral gas in the chamber. Also, both the electrons and positive ions are constrained by said axially symmetric magnetic field t-o helical paths I of which the axes are parallel to the axis of the chamber .11 and said orifice 34.
Several parameters are mutually interrelated and tend to be interdependent in the operation of the plasma generation chamber. For maximum efi'iciency the magnetic fieldthat passes through the plasma generation chamber 24 is adjusted so that the cyclotron frequency for electrons (Fc) in the chamber is equal to that of the operating frequency (Fm) of the'magnetron as given by the following relation:
where:
Under-these conditions, electrons in the plasma gen- -eration chamber 24receive the major portion of the energy from the electrical field, and a plasma'can'be produced with the least energy. Withappropriately adthe ion" density (n) will increase until the electron plasma -justedt power input and gas pressure, in, the plasma,
"frequency (Fp) approaches the :mag-netron frequency {(Fm) as indicated by the followingr'ela'tion:
the focusing effect of the axially symmetric magnetic field acting in cooperation with the flow of gas through the orifice caused by the lower pressure (below approximately mm.) in the evacuated region contained by the housing 11. The gas flow is essential to the production of the electrical neutral plasma since the electrical extraction methods employed conventionally cause charge separation and the production of a positive ion beam. It will be appreciated that the short section of tubing 33 is provided to reduce the rate of gas flow from the plasma generation chamber 24 establishing the indicated pressure difierential thereacross. Due to the constraint afforded by the magnetic field the orifice structure will have little effect on the plasma.
It will be noted that the aforementioned extraction method effectively screens out most of the neutral particles as the plasma is selectively focused and flows through the orifice 34. The probability that a neutral particle following its usual random path has of escaping through such an orifice is small compared to that of a plasma particle focused as described by an axially symmetric magnetic field. The few gas molecules that escape through the orifice will diffuse randomly into the evacuated region as they are not effected by the magnetic field therein, and thus the extracted focused plasma is further freed from contamination by neutral particles as it emerges from the orifice into the housing. In addition, the electron beam usually associated with the production of a plasma is eliminated in the present invention by the extraction method employed; nevertheless, the electrons required to provide electrical neutrality are entrained and carried along by the positive ion content of the plasma. Hence, in the low pressure region of the housing 11 there is provided a low temperature uncontaminated plasma, focused along the axis of the magnetic field, without the presence of an electron beam or neutral particles and which can be utilized for various purposes therein.
While the invention has been disclosed with respect to a single preferred embodiment, it will be apparent to those skilled in the art that numerous variations and modifications may be made within the spirit and scope of the invention and thus it is not intended to limit the invention except as defined in the following claims.
What is claimed is:
l. A plasma generator comprising in combination a plasma generation chamber having an exit orifice, a source for introducing gas to said chamber, means for ionizing gas in said chamber wherein a plasma is formed, magnetic field means for focusing said plasma, and means for establishing a pressure differential across said orifice whereby said plasma is focused and extracted through said orifice by said magnetic field in cooperation with said pressure differential.
2. A plasma generator comprising in combination an evacuated housing, a plasma generation chamber having an exit orifice communicating with said evacuated housing, a source for introducing gas to said chamber, thereby :festablishing :a pressure :idifierential racross sai'd orifice,
means establishing :an axially asymmetric :magnetic F. field :ncrrnal torsaid orifice,aandameanslfor:establishingthigh s'frequency electrical ifields 2 in said rchamber :for-i-onizing sgas in said chamber ito :form :;a plasma that :is :focused 13.1111 :extractdtthroughnsaid -;orifice by' zsaidfmagnetict: field :actingain cooperation withusaidrpressure differential.
13. 1A ,plasma .1 generator comprising in 1 combination tan evacuated. housing, ;a plasma -,generation chamber having an :exit :orifice icommunicat-ing with .said evacuated l1ousing, a variable :pressure source1for introducing :gas -to .said :,chamber zthereby establishing ;:a' pressure differ- -.enti'al across :said .x'mrifice, magnetic Jzfield .means :estabdishing an =ax-ially asymmetric magnetic field normal 1 to said orifice of controlled intensity, arid-.meanstproducing ::and coupling thigh zfrequency 1 electromagnetic ,rradiration. into 1 said chambjer=with theafrequency thereof :substantially equal to the cyclotron frequency of electrons in said chamber and to the electron plasma frequency for maximized ionization efficiency, whereby a plasma is formed in said chamber and is magnetically focused and pressure propelled through said orifice.
4. A plasma generator comprising in combination an evacuated housing, a plasma generation chamber having an exit orifice communicating with said evacuated housing, a source for introducing gas to said chamber thereby establishing a pressure differential across said orifice, a solenoid element adapted for energization to establish a magnetic field directed axially through said orifice, and wave guide means terminating in said chamber whereby very high radio frequency excitation applied to said wave guide excites and ionizes gas molecules in said chamber producing a plasma which thenceforth is focused and extracted through said orifice by said magnetic field acting in cooperation with said pressure dif ferential.
5. A plasma generator comprising in combination an evacuated housing, a wave guide element having an exit orifice communicating with said evacuated housing, a gas tight partition pervious to radio frequency radiation disposed within said wave guide forming a plasma generation chamber proximal to said exit orifice, a source for introducing gas to said chamber thereby establishing a pressure differential across said orifice, means for establishing an axially symmetric magnetic field normal to said orifice, and high frequency generating means energizing said wave guide to cause ionization of gas in said plasma generation chamber wherein a plasma may be formed and thenceforth focused and extracted through said orifice by said magnetic field acting in cooperation with said pressure differential.
6. A plasma generator comprising in combination an evacuated housing, a wave guide transpiercing one wall of saidevacuated housing, said wave guide having an exit orifice opening into said evacuated housing, a gas tight partition pervious to radio frequency disposed within the end region of said wave guide extending into said evacuated housing forming a plasma generation chamber proximal to said exit orifice, a source for introducing gas to said chamber thereby establishing a pressure differential across said orifice, magnetic field means for establishing an axially symmetric magnetic field normal to said orifice, and radio frequency generating means coupled to said wave guide for ionizing gas in said chamber wherein a plasma may be formed and thenceforth be focused and extracted through said orifice by said magnetic field acting in cooperation with said pressure differential.
7. A plasma generator comprising in combination an .wave guide proximal tossaid exit orifice thereby forming I a plasma generation chamber communicatingiwithsaid vessel, a source for introducing gas to said chamber thereby establishing a'pressure difierential across said orifice, a solenoid disposed coaxially with said vessel to provide an axially symmetric magnetic field in said vessel and said chamber normal to said orifice, generating means for producing high frequency electromagnetic radiation coupled to said wave guide through a matching section whereby said wave guide is energized causing ionization of the gas molecules in said plasma generation chamber to establish a plasma therein, which plasma is focused and extracted through said orifice by said magnetic field acting in cooperation with said pressure differential.
8. In a method for providing an uncontaminated plasma, the steps comprising producing a contaminated plas- 10 plasma beam.
ma in a defined region having an exit orifice, and extracting said plasma by focusing said plasma along the axis of said orifice with. an axially symmetric magnetic field and simultaneously providing a decreasing gas pressure gradient across said orifice whereby said plasma is selectively extracted from said'defined region through said orifice as a Well defined plasma beam and any neutral gas particles emerging from said orifice diffuse in a randomly indiscrete manner so as to separate from said References Cited in the file of this patent UNITED STATES PATENTS 1 2,400,557 Lawlor May 21, 1946 2,545,595 Alvarez, Mar. 20, 1951 2,582,216 -Koppius Jan. 15, 1952
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Cited By (44)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2880337A (en) * 1958-01-02 1959-03-31 Thompson Ramo Wooldridge Inc Particle acceleration method and apparatus
US2892114A (en) * 1958-05-06 1959-06-23 Wallace D Kilpatrick Continuous plasma generator
US2919370A (en) * 1958-10-28 1959-12-29 Plasmadyne Corp Electrodeless plasma torch and method
US2920235A (en) * 1958-07-24 1960-01-05 Persa R Bell Method and apparatus for producing intense energetic gas discharges
US2927232A (en) * 1958-07-15 1960-03-01 John S Luce Intense energetic gas discharge
US2928966A (en) * 1958-07-09 1960-03-15 Rodger V Neidigh Arc discharge and method of producing the same
US2929951A (en) * 1958-04-28 1960-03-22 Finkelstein David Ion-stabilized electron induction accelerator
US2946914A (en) * 1958-06-16 1960-07-26 Stirling A Colgate Apparatus for producing and manipulating plasmas
US2946919A (en) * 1956-10-03 1960-07-26 Csf Ion sources using a high-frequency field
US2958803A (en) * 1957-09-09 1960-11-01 Bell Telephone Labor Inc Gas discharge protector for vacuum systems
US2969475A (en) * 1956-07-14 1961-01-24 Berghaus Elektrophysik Anst Method and installation for carrying out glow discharge processes
US2969480A (en) * 1958-05-03 1961-01-24 Commissariat Energie Atomique Ion sources
US2971122A (en) * 1958-06-23 1961-02-07 Univ California High-power magnetron
US2992345A (en) * 1958-03-21 1961-07-11 Litton Systems Inc Plasma accelerators
US3003061A (en) * 1956-04-02 1961-10-03 Berghaus Elektrophysik Anst Electric discharges in gases
US3014857A (en) * 1958-09-02 1961-12-26 James D Gow Plasma device
US3015618A (en) * 1958-06-30 1962-01-02 Thomas H Stix Apparatus for heating a plasma
US3020431A (en) * 1957-11-20 1962-02-06 American Radiator & Standard Ion source and plasma generator
US3026447A (en) * 1959-06-10 1962-03-20 Gen Dynamics Corp Plasma containing device
US3029635A (en) * 1956-07-09 1962-04-17 Amalgamated Growth Ind Inc High-temperature testing apparatus
US3032490A (en) * 1958-04-28 1962-05-01 Simon Albert Destruction of neutral particles in a device for producing a high density plasma
US3041824A (en) * 1956-05-01 1962-07-03 Amalgamated Growth Ind Inc Propulsion system
US3055213A (en) * 1959-02-24 1962-09-25 Plasmadyne Corp Wind tunnel apparatus making use of the momentum of electrical plasma
US3063291A (en) * 1959-09-24 1962-11-13 Childs James Howard High-vacuum condenser tank for ion rocket tests
US3084281A (en) * 1956-11-30 1963-04-02 Carroll B Mills Ion source
US3089831A (en) * 1959-08-13 1963-05-14 Alan C Kolb Method of producing high gas temperatures
US3105803A (en) * 1958-01-15 1963-10-01 Space Technology Lab Inc Gas confining apparatus
US3113088A (en) * 1959-07-27 1963-12-03 Space Technology Lab Inc Apparatus for the generation and confinement of high kinetic energy gases
US3120476A (en) * 1958-04-28 1964-02-04 Richard F Post Pyrotron process and apparatus utilizing enhancement principle
US3150483A (en) * 1962-05-10 1964-09-29 Aerospace Corp Plasma generator and accelerator
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US3156090A (en) * 1961-09-18 1964-11-10 Harold R Kaufman Ion rocket
US3174068A (en) * 1959-05-14 1965-03-16 Csf Plasma confining device
US3177654A (en) * 1961-09-26 1965-04-13 Ryan Aeronautical Company Electric aerospace propulsion system
US3225236A (en) * 1961-01-03 1965-12-21 Trw Inc Propulsion arrangement
US3256687A (en) * 1958-07-31 1966-06-21 Avco Mfg Corp Hydromagnetically operated gas accelerator propulsion device
US3264508A (en) * 1962-06-27 1966-08-02 Lai William Plasma torch
US3265896A (en) * 1961-06-30 1966-08-09 Atomic Energy Authority Uk Cold cathode neutron generator tube
US3283205A (en) * 1961-06-01 1966-11-01 Bolt Harold E De Shifting arc plasma system
US3286187A (en) * 1961-10-16 1966-11-15 Minnesota Mining & Mfg Ion source utilizing a spherically converging electric field
US4139772A (en) * 1977-08-08 1979-02-13 Western Electric Co., Inc. Plasma discharge ion source
US4472174A (en) * 1983-04-25 1984-09-18 Raymond L. Chuan Method and apparatus for providing and using RF generated plasma for particle charging in electrostatic precipitation
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Cited By (47)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3003061A (en) * 1956-04-02 1961-10-03 Berghaus Elektrophysik Anst Electric discharges in gases
US3041824A (en) * 1956-05-01 1962-07-03 Amalgamated Growth Ind Inc Propulsion system
US3029635A (en) * 1956-07-09 1962-04-17 Amalgamated Growth Ind Inc High-temperature testing apparatus
US2969475A (en) * 1956-07-14 1961-01-24 Berghaus Elektrophysik Anst Method and installation for carrying out glow discharge processes
US2946919A (en) * 1956-10-03 1960-07-26 Csf Ion sources using a high-frequency field
US3084281A (en) * 1956-11-30 1963-04-02 Carroll B Mills Ion source
US2958803A (en) * 1957-09-09 1960-11-01 Bell Telephone Labor Inc Gas discharge protector for vacuum systems
US3020431A (en) * 1957-11-20 1962-02-06 American Radiator & Standard Ion source and plasma generator
US2880337A (en) * 1958-01-02 1959-03-31 Thompson Ramo Wooldridge Inc Particle acceleration method and apparatus
US3105803A (en) * 1958-01-15 1963-10-01 Space Technology Lab Inc Gas confining apparatus
US2992345A (en) * 1958-03-21 1961-07-11 Litton Systems Inc Plasma accelerators
US2929951A (en) * 1958-04-28 1960-03-22 Finkelstein David Ion-stabilized electron induction accelerator
US3120476A (en) * 1958-04-28 1964-02-04 Richard F Post Pyrotron process and apparatus utilizing enhancement principle
US3032490A (en) * 1958-04-28 1962-05-01 Simon Albert Destruction of neutral particles in a device for producing a high density plasma
US2969480A (en) * 1958-05-03 1961-01-24 Commissariat Energie Atomique Ion sources
US2892114A (en) * 1958-05-06 1959-06-23 Wallace D Kilpatrick Continuous plasma generator
US2946914A (en) * 1958-06-16 1960-07-26 Stirling A Colgate Apparatus for producing and manipulating plasmas
US2971122A (en) * 1958-06-23 1961-02-07 Univ California High-power magnetron
US3015618A (en) * 1958-06-30 1962-01-02 Thomas H Stix Apparatus for heating a plasma
US2928966A (en) * 1958-07-09 1960-03-15 Rodger V Neidigh Arc discharge and method of producing the same
US2927232A (en) * 1958-07-15 1960-03-01 John S Luce Intense energetic gas discharge
US2920235A (en) * 1958-07-24 1960-01-05 Persa R Bell Method and apparatus for producing intense energetic gas discharges
US3256687A (en) * 1958-07-31 1966-06-21 Avco Mfg Corp Hydromagnetically operated gas accelerator propulsion device
US3014857A (en) * 1958-09-02 1961-12-26 James D Gow Plasma device
US2919370A (en) * 1958-10-28 1959-12-29 Plasmadyne Corp Electrodeless plasma torch and method
US3055213A (en) * 1959-02-24 1962-09-25 Plasmadyne Corp Wind tunnel apparatus making use of the momentum of electrical plasma
US3174068A (en) * 1959-05-14 1965-03-16 Csf Plasma confining device
US3026447A (en) * 1959-06-10 1962-03-20 Gen Dynamics Corp Plasma containing device
US3113088A (en) * 1959-07-27 1963-12-03 Space Technology Lab Inc Apparatus for the generation and confinement of high kinetic energy gases
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