US3678323A - Hydrogen ion beam generating electrode - Google Patents
Hydrogen ion beam generating electrode Download PDFInfo
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- US3678323A US3678323A US96145A US3678323DA US3678323A US 3678323 A US3678323 A US 3678323A US 96145 A US96145 A US 96145A US 3678323D A US3678323D A US 3678323DA US 3678323 A US3678323 A US 3678323A
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- hollow tube
- electrode
- tube
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J27/00—Ion beam tubes
- H01J27/02—Ion sources; Ion guns
- H01J27/08—Ion sources; Ion guns using arc discharge
Definitions
- the electrode By controlling the temperature of the electrode, its output is selectable from molecular hydrogen at temperatures below 1,500 K. to essentially pure monoatomic hydrogen for temperatures near or above 2,800 K.
- the combination of the electrode output and the source arc then allows a range of selection in ion source output composition of 1-1", 1-1" and 11* ⁇ . Above 2,800 K., the source output is essentially pure 1-1", from are ionization of monoatomic hydrogen.
- the inventive electrode for a hydrogen ion source features a hollow tube of tungsten or other suitable metal for producing I-l exclusively, or a wide range of combinations of a mixed beam of H Hf, and H
- the tube is provided in the central portion thereof with mesh or wool of tungsten or other suitable metal and has a conically wound heating element concentrically about the beam output end of the tube for variably heating the tube for effecting the dissociation of hydrogen gas into atomic hydrogen.
- The are ionizes molecular hydrogen into various mixtures of IF, Hf, and H or atomic hydrogen into I-I Therefore, it is an object of this invention to provide an electrode for the arc discharge of hydrogen
- a further object of the invention is to provide a means for dissociating molecular hydrogen gas to atomic hydrogen.
- Another object of the invention is to provide a cathode for a hydrogen ion beam source with selectable beam composition.
- Another object of the invention is to provide a cathode for a hydrogen ion source utilizing a hollow tungsten tube for producing I-I exclusively, or a wide range of combinations of a mixed beam of H H and Hf.
- Another object of the invention is to provide a hydrogen ion beam generating electrode which utilizes a hollow tungsten tube having a tungsten mesh in the central portion thereof and surrounded at the beam output end thereof with a conically wound heating element.
- FIG. 1 is a plan view, having a portion thereof cut away, illustrating an embodiment of the invention
- FIG. 2 illustrates a portion of another embodiment of the inventive cathode
- FIG. 3 is a graph showing tungsten temperature versus the percent of pure monoatomic hydrogen out.
- FIG 1 The embodiment of the invention illustrated in FIG 1 comprises an evacuated container (only a portion being illustrated) which houses a hollow tungsten tube or cylinder 11, the central portion of tube 11 containing tungsten mesh or wool 12. If desired the tube 11 and mesh 12 can be made of either tantalum, molybdenum or rhenium or combinations thereof.
- a conically wound heating element indicated at 13 is concentrically spaced about the beam output end 14 of the tube 11.
- the opposite end 15 of tube 11 is formed in an inverted funnel shape through which molecular hydrogen (H as indicated by the arrow 16, is directed into tube 11, the molecular hydrogen 16 being supplied from a source not shown.
- Heating element 13 is connected through a variable switch or rheostat 17 to a power supply 18.
- the temperature within tube 11 increases so that the hydrogen gas 16 entering the tube 11 through end portion 15 thereof tends to dissociate into atomic hydrogen.
- hydrogen in the output end 14 of the tube 11 tends to become almost entirely atomic hydrogen (H) due to thermodynamic dissociation.
- a concentric electrode 19 positioned near the end 14 of the tube 11 and coaxially aligned therewith is charged with a potential by a power supply 20 for creating an electric field between the electrode 19 and the tube 11.
- the electrode 19 tends to draw a hydrogen are indicated at 21 from the output end 14 of tube 11; when the are 21 is drawn in, nearly pure atomic hydrogen, mainly H ions, is produced.
- This feature of an arc plasma consisting of essentially H can be applied in any are type ion source to change the source ion output to nearly pure I-I ions.
- FIG. 2 illustrates a partial alternate embodiment of the inventive apparatus wherein a hollow tungsten tube 25, having a tungsten mesh or wool central portion 26 and an inverted funnel-like hydrogen gas inlet end portion 27, is located eoaxially within a hollow outer tube or cylinder 28 and electrically connected therewith at the open beam output end thereof as indicated by leads 29, so that tubes 25 and 28 can conduct a relatively high current therethrough for directly heating the hydrogen gas passing through the tube 25.
- the tungsten tube 25 and outer tube 28 are located within an evacuated housing or casing 30, and aligned with a concentric electrode as in the FIG. 1 embodiment.
- Outer hollow casing 28 is connected through a variable control means 31 to an electrical power supply as indicated at 32.
- FIG. 3 is a graph of tungsten temperature (T versus the percent of pure monoatomic hydrogen (%H output expected from the hollow cathode 11 of FIG. 1, for example.
- T tungsten temperature
- %H output expected from the hollow cathode 11 of FIG. 1, for example.
- the beam composition from the output end 14 of the tube rises in its percentage of H until a limit is reached at approximately 2,800 l(., the percentage H being indicated as 93 percent at this temperature.
- tungsten While it is possible to use materials other than tungsten to form the cathode 11, in general materials other than tungsten will require a temperature higher than 2,800 K. to achieve substantially over percent ionized monoatomic hydrogen output. As pointed out above, while tungsten has been specifically described regarding the tube and mesh, tantalum, molybdenum or rhenium may be utilized for either or for both of these elements.
- present invention provides a cathode for generating a hydrogen ion beam of selected composition.
- a cathode for generating a hydrogen ion beam of selected composition.
- its output is selectable from molecular hydrogen at temperatures below 1,500 K. to essentially pure monoatomic hydrogen for temperatures near 2,800 K.
- the ion composition in the source are then follows from a mixture of H", I-I and H; for lower heater temperatures to nearly pure I-l for temperatures near or above 2,800 K. Since the beam composition produced by the inventive ion source can be adjustably controlled, it is particularly useful in energetic beam production for controlled thermonuclear reactors, for example.
- An electrode for generating a hydrogen ion beam of selected composition comprising: a hollow tube means selected from the group consisting of tungsten, tantalum, molybdenum and rhenium, means through which molecular hydrogen gas is directed into said hollow tube means for dissociation thereof in said tube means, and means for heating said hollow tube means positioned around and in spaced relation to at least a portion of said tube means, said tube means containing metallic mesh in the central portion thereof, said mesh being selected from the group consisting of tungsten, tantalum, molybdenum and rhenium.
- heating means comprises a conically wound heating element concentrically spaced about at least a portion of said hollow tube means, and means for adjustably controlling the temperature of said heating element.
- heating means comprises a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means.
- said gas direct ing means includes an end portion of said hollow tube means having an inverted funnel-shaped configuration.
- said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced;
- said heating means includes a conically heating element concentrically spaced about said central portion and said open beam output end of said hollow tube means, and means for adjustably controlling the temperature of said heating element; and wherein said hollow tube means and said heating element are positioned in an evacuated housing means and in coaxial alignment with a concentric electrode means positioned in spaced relationship with respect to said open beam output end of said hollow tube means, and means for charging said concentric electrode means with a potential for creating an electric are between said electrode means and said open beam output end of said hollow tube means.
- said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced; wherein said heating means includes a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith at said open beam output end, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means, said tubelike means being positioned within an evacuated housing means.
Abstract
A hollow metallic electrode having a metallic mesh in the central portion thereof and a variable temperature heater for generating a hydrogen ion beam. By controlling the temperature of the electrode, its output is selectable from molecular hydrogen at temperatures below 1,500* K. to essentially pure monoatomic hydrogen for temperatures near or above 2,800* K. The combination of the electrode output and the source arc then allows a range of selection in ion source output composition of H , H 2 and H 3. Above 2,800* K., the source output is essentially pure H , from arc ionization of monoatomic hydrogen.
Description
United States Patent Osher et a1.
15] 3,678,323 [451 July 18, 1972 [54] HYDROGEN ION BEAM GENERATING ELECTRODE [72] Inventors: John E. Osher; John D. Kinney, both of Alamo; James F. Stelnhaus, Livermore, all of Calif.
[21] Appl. No.: 96,145
[52] US. Cl ..313/231, 313/63, 313/211, 313/217, 313/305, 313/311, 313/D1G. 8
[51] Int. Cl. ..H01j 17/26 [58] FieldofSearch ..313/2l1,305,231,31l,2l7, 313/218, 63, DIG. 8
[5 6] References Cited UNITED STATES PATENTS 2,975,277 3/1961 Von Ardenne ..3l3/23l X 3,156,842 11/1964 McClure ..3 1 3/63 3,201,635 8/1965 Carter ....313/231 X 3,320,475 5/1967 Boring ...313/D1G. 8 3,515,932 6/1970 King ...313/D1G. 8 3,531,673 9/1970 Paquette ..3 1 3/2 1 7 X Primary Examiner-Alfred L. Brody Attorney-Roland A. Anderson [57] ABSTRACT A hollow metallic electrode having a metallic mesh in the central portion thereof and a variable temperature heater for generating a hydrogen ion beam. By controlling the temperature of the electrode, its output is selectable from molecular hydrogen at temperatures below 1,500 K. to essentially pure monoatomic hydrogen for temperatures near or above 2,800 K. The combination of the electrode output and the source arc then allows a range of selection in ion source output composition of 1-1", 1-1" and 11*}. Above 2,800 K., the source output is essentially pure 1-1", from are ionization of monoatomic hydrogen.
7 Clains, 3 Drawing Figures ,20 POWER POWER SUPPLY SUPPLY PATENYED JUL 1 81972 POWER SUPPLY l l l I500'K 2800K TH Fig. 3
INVENTORS. John E. Osher John D. Kinney James FSfeinhaus BY ATTORNEY.
SUPPLY CONTROL Rw E 0 MU S 9 2 Ma R 5 2 E 2, 3 w m /m 6 9 2 E n U M T E a m m /A L H A V HYDROGEN ION BEAM GENERATING ELECTRODE BACKGROUND OF THE INVENTION SUMMARY OF THE INVENTION The inventive electrode for a hydrogen ion source features a hollow tube of tungsten or other suitable metal for producing I-l exclusively, or a wide range of combinations of a mixed beam of H Hf, and H The tube is provided in the central portion thereof with mesh or wool of tungsten or other suitable metal and has a conically wound heating element concentrically about the beam output end of the tube for variably heating the tube for effecting the dissociation of hydrogen gas into atomic hydrogen. The are ionizes molecular hydrogen into various mixtures of IF, Hf, and H or atomic hydrogen into I-I Therefore, it is an object of this invention to provide an electrode for the arc discharge of hydrogen ion beam source.
A further object of the invention is to provide a means for dissociating molecular hydrogen gas to atomic hydrogen.
Another object of the invention is to provide a cathode for a hydrogen ion beam source with selectable beam composition.
Another object of the invention is to provide a cathode for a hydrogen ion source utilizing a hollow tungsten tube for producing I-I exclusively, or a wide range of combinations of a mixed beam of H H and Hf.
Another object of the invention is to provide a hydrogen ion beam generating electrode which utilizes a hollow tungsten tube having a tungsten mesh in the central portion thereof and surrounded at the beam output end thereof with a conically wound heating element.
Other objects of the invention, not specifically set forth above, will become readily apparent from the following description and accompanying drawings.
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a plan view, having a portion thereof cut away, illustrating an embodiment of the invention;
FIG. 2 illustrates a portion of another embodiment of the inventive cathode; and
FIG. 3 is a graph showing tungsten temperature versus the percent of pure monoatomic hydrogen out.
DESCRIPTION OF THE INVENTION The embodiment of the invention illustrated in FIG 1 comprises an evacuated container (only a portion being illustrated) which houses a hollow tungsten tube or cylinder 11, the central portion of tube 11 containing tungsten mesh or wool 12. If desired the tube 11 and mesh 12 can be made of either tantalum, molybdenum or rhenium or combinations thereof. A conically wound heating element indicated at 13 is concentrically spaced about the beam output end 14 of the tube 11. The opposite end 15 of tube 11 is formed in an inverted funnel shape through which molecular hydrogen (H as indicated by the arrow 16, is directed into tube 11, the molecular hydrogen 16 being supplied from a source not shown. Heating element 13 is connected through a variable switch or rheostat 17 to a power supply 18. By increasing the current in the heating coil 13, the temperature within tube 11 increases so that the hydrogen gas 16 entering the tube 11 through end portion 15 thereof tends to dissociate into atomic hydrogen. As the temperature of the tungsten tube 11 approaches 2,800 K., hydrogen in the output end 14 of the tube 11 tends to become almost entirely atomic hydrogen (H) due to thermodynamic dissociation. A concentric electrode 19 positioned near the end 14 of the tube 11 and coaxially aligned therewith is charged with a potential by a power supply 20 for creating an electric field between the electrode 19 and the tube 11. The electrode 19 tends to draw a hydrogen are indicated at 21 from the output end 14 of tube 11; when the are 21 is drawn in, nearly pure atomic hydrogen, mainly H ions, is produced. This feature of an arc plasma consisting of essentially H can be applied in any are type ion source to change the source ion output to nearly pure I-I ions.
FIG. 2 illustrates a partial alternate embodiment of the inventive apparatus wherein a hollow tungsten tube 25, having a tungsten mesh or wool central portion 26 and an inverted funnel-like hydrogen gas inlet end portion 27, is located eoaxially within a hollow outer tube or cylinder 28 and electrically connected therewith at the open beam output end thereof as indicated by leads 29, so that tubes 25 and 28 can conduct a relatively high current therethrough for directly heating the hydrogen gas passing through the tube 25. The tungsten tube 25 and outer tube 28 are located within an evacuated housing or casing 30, and aligned with a concentric electrode as in the FIG. 1 embodiment. Outer hollow casing 28 is connected through a variable control means 31 to an electrical power supply as indicated at 32. By directly heating the hydrogen gas, indicated by the arrows 33, greater system efficiencies can be obtained.
FIG. 3 is a graph of tungsten temperature (T versus the percent of pure monoatomic hydrogen (%H output expected from the hollow cathode 11 of FIG. 1, for example. As the hollow tungsten cathode or tube 11 raises in temperature by the heating coils 13 the beam composition from the output end 14 of the tube rises in its percentage of H until a limit is reached at approximately 2,800 l(., the percentage H being indicated as 93 percent at this temperature.
While it is possible to use materials other than tungsten to form the cathode 11, in general materials other than tungsten will require a temperature higher than 2,800 K. to achieve substantially over percent ionized monoatomic hydrogen output. As pointed out above, while tungsten has been specifically described regarding the tube and mesh, tantalum, molybdenum or rhenium may be utilized for either or for both of these elements.
It has thus been seen that present invention provides a cathode for generating a hydrogen ion beam of selected composition. By controlling the temperature of the cathode, its output is selectable from molecular hydrogen at temperatures below 1,500 K. to essentially pure monoatomic hydrogen for temperatures near 2,800 K. The ion composition in the source are then follows from a mixture of H", I-I and H; for lower heater temperatures to nearly pure I-l for temperatures near or above 2,800 K. Since the beam composition produced by the inventive ion source can be adjustably controlled, it is particularly useful in energetic beam production for controlled thermonuclear reactors, for example.
While particular embodiments of the invention have been illustrated and described, modifications will become apparent to those skilled in the art, and it is intended to cover in the appended claims all such modification as come within the spirit and scope of the invention.
What we claim is:
1. An electrode for generating a hydrogen ion beam of selected composition comprising: a hollow tube means selected from the group consisting of tungsten, tantalum, molybdenum and rhenium, means through which molecular hydrogen gas is directed into said hollow tube means for dissociation thereof in said tube means, and means for heating said hollow tube means positioned around and in spaced relation to at least a portion of said tube means, said tube means containing metallic mesh in the central portion thereof, said mesh being selected from the group consisting of tungsten, tantalum, molybdenum and rhenium.
2. The electrode defined in claim 1, wherein said hollow tube means and said heating means are positioned in an evacuated housing means and in coaxial alignment with a concentric electrode means positioned in spaced relationship with said hollow tube means, and means for charging said electrode means with a potential for creating an electric are between said electrode means and said hollow tungsten tube means.
3. The electrode defined in claim 1, wherein said heating means comprises a conically wound heating element concentrically spaced about at least a portion of said hollow tube means, and means for adjustably controlling the temperature of said heating element.
4. The electrode defined in claim 1, wherein said heating means comprises a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means.
5. The electrode defined in claim 1, wherein said gas direct ing means includes an end portion of said hollow tube means having an inverted funnel-shaped configuration.
6. The electrode defined in claim 1, wherein said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced; wherein said heating means includes a conically heating element concentrically spaced about said central portion and said open beam output end of said hollow tube means, and means for adjustably controlling the temperature of said heating element; and wherein said hollow tube means and said heating element are positioned in an evacuated housing means and in coaxial alignment with a concentric electrode means positioned in spaced relationship with respect to said open beam output end of said hollow tube means, and means for charging said concentric electrode means with a potential for creating an electric are between said electrode means and said open beam output end of said hollow tube means.
7. The electrode defined in claim 1, wherein said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced; wherein said heating means includes a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith at said open beam output end, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means, said tubelike means being positioned within an evacuated housing means.
Claims (7)
1. An electrode for generating a hydrogen ion beam of selected composition comprising: a hollow tube means selected from the group consisting of tungsten, tantalum, molybdenum and rhenium, means through which molecular hydrogen gas is directed into said hollow tube means for dissociation thereof in said tube means, and means for heating said hollow tube means positioned around and in spaced relation to at least a portion of said tube means, said tube means containing metallic mesh in the central portion thereof, said mesh being selected from the group consisting of tungsten, tantalum, molybdenum and rhenium.
2. The electrode defined in claim 1, wherein said hollow tube means and said heating means are positioned in an evacuated housing means and in coaxial alignment with a concentric electrode means positioned in spaced relationship with said hollow tube means, and means for charging said electrode means with a potential for creating an electric arc between said electrode means and said hollow tungsten tube means.
3. The electrode defined in claim 1, wherein said heating means comprises a conically wound heating element concentrically spaced about at least a portion of said hollow tube means, and means for adjustably controlling the temperature of said heating element.
4. The electrode defined in claim 1, wherein said heating means comprises a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means.
5. The electrode defined in claim 1, wherein said gas directing means includes an end portion of said hollow tube means having an inverted funnel-shaped configuration.
6. The electrode defined in claim 1, wherein said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced; wherein said heating means includes a conically heating element concentrically spaced about said central portion and said open beam output end of said hollow tube means, and means for adjustably controlling the temperature of said heating element; and wherein said hollow tube means and said heating element are positioned in an evacuated housing means and in coaxial alignment with a concentric electrode means positioned in spaced relationship with respect to said open beam output end of said hollow tube means, and means for charging said concentric electrode means with a potential for creating an electric arc between said electrode means and said open beam output end of said hollow tube means.
7. The electrode defined in claim 1, wherein said hollow tube means includes an open beam output end and said gas directing means comprises an inverted funnel-shaped inlet end through which molecular hydrogen gas is adapted to be introduced; wherein said heating means includes a tube-like means positioned coaxially about said hollow tube means and electrically connected therewith at said open beam output end, and means for adjustably controlling the temperature of said tube-like means and said hollow tube means, said tube-like means being positioned within an evacuated housing means.
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US9614570A | 1970-12-08 | 1970-12-08 |
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US3678323A true US3678323A (en) | 1972-07-18 |
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US96145A Expired - Lifetime US3678323A (en) | 1970-12-08 | 1970-12-08 | Hydrogen ion beam generating electrode |
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5382866A (en) * | 1992-05-06 | 1995-01-17 | Gesellschaft Fur Schwerionenforschung Mbh | Method of focusing a charged particle beam and plasma lens therefor |
US20160225571A1 (en) * | 2013-08-12 | 2016-08-04 | The Government Of The United States Of America, As Represented By The Secretary Of The Navy | Chemically Stable Visible Light Photoemission Electron Source |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2975277A (en) * | 1955-05-10 | 1961-03-14 | Vakutronik Veb | Ion source |
US3156842A (en) * | 1962-10-08 | 1964-11-10 | Gordon W Mcclure | Gas ionizer |
US3201635A (en) * | 1962-03-07 | 1965-08-17 | Arlen F Carter | Method and apparatus for producing a plasma |
US3320475A (en) * | 1963-04-30 | 1967-05-16 | Gen Electric | Nonthermionic hollow cathode electron beam apparatus |
US3515932A (en) * | 1967-04-27 | 1970-06-02 | Hughes Aircraft Co | Hollow cathode plasma generator |
US3531673A (en) * | 1968-06-04 | 1970-09-29 | Varo | Two-piece arc electrode having a plurality of heat-conducting paths between the arc tip and the tip holder |
-
1970
- 1970-12-08 US US96145A patent/US3678323A/en not_active Expired - Lifetime
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2975277A (en) * | 1955-05-10 | 1961-03-14 | Vakutronik Veb | Ion source |
US3201635A (en) * | 1962-03-07 | 1965-08-17 | Arlen F Carter | Method and apparatus for producing a plasma |
US3156842A (en) * | 1962-10-08 | 1964-11-10 | Gordon W Mcclure | Gas ionizer |
US3320475A (en) * | 1963-04-30 | 1967-05-16 | Gen Electric | Nonthermionic hollow cathode electron beam apparatus |
US3515932A (en) * | 1967-04-27 | 1970-06-02 | Hughes Aircraft Co | Hollow cathode plasma generator |
US3531673A (en) * | 1968-06-04 | 1970-09-29 | Varo | Two-piece arc electrode having a plurality of heat-conducting paths between the arc tip and the tip holder |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5382866A (en) * | 1992-05-06 | 1995-01-17 | Gesellschaft Fur Schwerionenforschung Mbh | Method of focusing a charged particle beam and plasma lens therefor |
US20160225571A1 (en) * | 2013-08-12 | 2016-08-04 | The Government Of The United States Of America, As Represented By The Secretary Of The Navy | Chemically Stable Visible Light Photoemission Electron Source |
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