U.S. patent number 3,760,225 [Application Number 05/260,236] was granted by the patent office on 1973-09-18 for high current plasma source.
This patent grant is currently assigned to The United States of America as represented by the United States Atomic. Invention is credited to William R. Baker, Kenneth W. Ehlers, Wulf B. Kunkel.
United States Patent |
3,760,225 |
Ehlers , et al. |
September 18, 1973 |
HIGH CURRENT PLASMA SOURCE
Abstract
A plasma source in which a plurality of sturdy filaments are
distributed around the perimeter of a truncated cylindrical
discharge chamber. A small area anode is situated axially at one
end of the chamber with an accel-decel extraction grid system at
the other end. A high current electron discharge pulse is
established between the filaments and anode and a puff of gas is
directed past the anode into the discharge chamber to be ionized to
form an arc plasma from which a high current beam is extracted and
directed by the extractor grids. The output contains a high
proportion of energetic neutrals suitable for use in fueling a
fusion reactor or other purpose.
Inventors: |
Ehlers; Kenneth W. (Alamo,
CA), Kunkel; Wulf B. (Berkeley, CA), Baker; William
R. (Orinda, CA) |
Assignee: |
The United States of America as
represented by the United States Atomic (Washington,
DC)
|
Family
ID: |
22988348 |
Appl.
No.: |
05/260,236 |
Filed: |
June 6, 1972 |
Current U.S.
Class: |
376/109;
315/111.31; 315/334; 376/128; 315/98; 315/167; 376/116 |
Current CPC
Class: |
H05H
1/48 (20130101) |
Current International
Class: |
H05H
1/24 (20060101); H05H 1/48 (20060101); H01j
007/24 (); H05h 001/00 () |
Field of
Search: |
;313/63
;315/111,167,334,98 ;176/1 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Demeo; Palmer C.
Claims
What we claim is:
1. In a high current plasma or ion source, the combination
comprising:
vessel means defining a generally cylindrical arc discharge chamber
and having a centrally apertured wall at one end together with a
mounting plate means at the other end defining a port for
extraction of ions;
electron emitter means including a plurality of refractory metal
filaments extending longitudinally in the outer perimeter area of
said chamber;
anode body means disposed in spaced insulated relation within the
aperture of said wall at one end of said vessel means;
gas source reservoir means including a conduit arranged to direct a
quantity of a selected gas about a perimeter of said anode body
into said discharge chamber; and
first power supply means for energizing said metal filaments to
cause emission of electrons therefrom and second power supply means
for applying a positive potential to said anode relative to said
filaments. thereby creating an arc discharge through the gas
directed into said chamber so as to create a plasma therein.
2. A high current plasma or ion source as defined in claim 1
wherein a vessel extension is attached to said mounting plate means
and ion extractor means are provided, said ion extractor means
comprising at least one apertured grid member disposed transversely
proximate said ion extractor port.
3. A high current plasma or ion source as defined in claim 2
wherein said ion extractor means comprises accel-decel grid
electrodes disposed in said vessel extension and power supply means
for energizing said grids so that a beam of energetic particles is
extracted from said plasma and is directed through the channel
defined by said vessel extension.
4. A source as defined in claim 3 wherein said filaments comprise
hairpin shaped wire filaments and the ends of said filaments are
supported in insulated sealed relation at said one vessel endwall,
said filaments being connected in a parallel circuit.
5. A source as defined in claim 4 wherein said anode body comprises
a circular plate disposed in coaxial spaced relation within the
aperture of aid one vessel endwall.
6. A source as defined in claim 4 wherein said anode body comprises
a hollow cylinder disposed coaxially within the aperture of said
one vessel endwall
7. A source as defined in claim 4 wherein said vessel extension is
provided with mounting means at the ion beams outlet end for
attaching said source to an injector port of a controlled
thermonuclear fusion reactor.
8. A source as defined in claim 7 wherein said gas source reservoir
means supplies a gas selected from the group consisting of
hydrogen, deuterium and tritium and mixtures thereof.
Description
BACKGROUND OF THE INVENTION
This invention was conceived or made in the course of Contract No.
W-7405-ENG-48 with the United States Atomic Energy Commission.
In nuclear fusion reactor practice certain modes of operation
require the use of high current energetic neutral particle sources.
For example, sources capable of delivering energetic particle
current densities of the order of 1 ampere/cm.sup.2 at energies of
up to 20 keV or more with a beam current which is relatively
uniform over a large extraction area may be required. Moreover
certain reactors such as the 2XII experiment require beam pulses
lengths of the order of 0.03 to 0.1 seconds (c.f. F. H. Coensgen et
al., "Plasma Containment" in the LRL 2XII Experiment, IAEA/CN/612
paper, Madison, Wis., June, 1971). Since ion extraction optics are
quite sensitive to plasma density, little variation in beam
intensity can be tolerated in order that the beam be usable in such
reactors. Therefore, sources not subject to fluctuations or noise
of the type and frequency encountered with most conventional
sources are needed.
SUMMARY OF THE INVENTION
This invention relates, generally, to devices for producing beams
of energetic particles and, more particularly, to a plasma source
for producing a uniformly distributed high current beam of
energetic particles.
A plasma source in accordance with the invention includes a vessel
defining a discharge chamberhaving a truncated cylindrical
configuration and an axial port opening in one endwall thereof. A
plurality of refractory metal filament wires are arranged at spaced
locations about the perimeter of the discharged chamber generally
parallel to the cylindrical wall portion of said vessel.
Preferably, such filaments are of a heavy generally hairpin
construction self supported from electrical connectors or insulated
seals secured to said ported endwall and arranged to pass a heavy
pulse heating current through said filaments to provide copious
electron emission therefrom. An anode body is disposed coaxially
within said port with a relatively small surface area proximate the
endwall surface level exposed within said chamber. Such anode is
supported in insulated relation to said endwall and is arranged for
application of a positive electrical potential so as to cause said
copious emission of electrons from the filament creating an
electrical discharge filling at least the portions of the discharge
chamber enclosed by said filaments. A conduit means is arranged to
direct gas, released in a relatively large volume by a puff valve
from an exterior source, about the periphery of said anode to enter
the electron discharge. The gas is ionized and heated by
interaction with the electrons forming a dense plasma body filling
the discharge chamber. Extractor electrode means arranged outwardly
from the second end of the discharge chamber are energized with a
relatively high voltage net potential thereupon extracting a high
current of positive ions from the discharge plasma. The ion current
has a uniform distribution across the extraction area and emerges,
e.g., in an extraction channel, as an ion beam with a very low
angle of divergence. Moreover, the ion beam which isproduced
contains a high proportion of energetic neutral particles due to
the high gas density existing in the extractor channel and thereby
being highly suitable for injection into the magnetic containment
field of a controlled fusion reactor to provide a high density
temperature reaction plasma therein. Accessory equipment including
pulsed filament, anode and extractor power supply means is also
provided for operating the plasma source.
Accordingly, it is an object of the invention to provide a high
beam current ion or plasma source in which the beam current is
relatively uniform over a large area.
Another object of the invention is to provide a high current
energetic particle source adapted for use in establishing a plasma
of high density and elevated temperature in a controlled fusion
reactor.
Still another object of the invention is to provide a plasma source
in which the beam has minimal modulation noise components.
Other objects and advantageous features of the invention will be
apparent in the following description and accompanying drawing of
which the single FIGURE is a longitudinal sectional view of the ion
or plasma source of the invention.
DETAILED DESCRIPTION OF THE INVENTION
As illustrated in the single FIGURE of the drawing, the ion source
of the invention comprises a generally cylindrical vessel 11
defining a truncated cylindrical arc discharge chamber 12. Vessel
11 includes a cylindrical tubular wall portion 13 with an endwall
portion 14 centrally apertured to receive anode and gas inlet
fixtures and secured to one end, i.e., the anode end thereof. More
specifically, wall portion 13 may be cut-away to provide an
enlarged shoulder portion 16 to receive endwall 14 with flange
portion 17 thereof bearing upon insulating gasket seal 18 which in
turn bears upon the end of wall portion 13. An O-ring sealing
member may also be similarly disposed between flange 17 and said
end of wall 13.
A plurality of hairpin type electron-emitter filaments 21 of
tungsten or other refractory metal are arranged in spaced relation
somewhat inwardly of and parallel to vessel wall 13, i.e.,
circumferentially in the outer perimeter region of chamber 12. It
has been found efficacious that no portion of the means for
supporting and supplying electrical current to such filaments
project within chamber 12. A convenient arrangement for supporting
filaments 21 is obtained by providing counterbores 22 in endwall
portion 14 with apertures 23 leading therefrom into chamber 12 at
spaced locations appropriate to accommodate the respective ends of
filaments 21. Cylindrical copper slug connectors, bored and crimped
at one end to receive and secure the ends of filaments 21 are
disposed in spaced relation within such counterbores 22. Relatively
shorter slug connectors 24 (one only shown) are secured to one
respective end of filaments 21 and the second ends of the slugs 24
are secured to an intermediate annular copper plate conductor 27
separated from endwall portion 14 by gasket 28 and O-ring seal
members 29. The other respective ends of filaments 21 similarly
secured and supported at one end of relatively longer slug
connectors 31 (one only shown) which connectors 31 project in
spaced relation through bores 32 matching with alternateones of
counterbores 22 and are sedured at the other end to an outermost
annular plate conductor 33. Plate conductor 33 may be insulated
from plate conductor 27 with an insulating gasket 34 disposed
therebetween. With the foregoing arrangement the filaments are
connected in parallel across plate conductors 27 and 33 which
provide a low resistance high current electrical connection
thereto. Machine screws 37 which pass through matching bores (not
shown) in plate conductors 27, 33 and flange 17 of endwall portion
14 to engage threaded holes in wall portion 13 may be used to
secure such members when assembled as described. Moreover, an
insulating sleeve (not shown) about the shanks of screws 37 and an
insulating washer 38 beneath the head of the screws may be used to
preserve the insulated relation therebetween or, alternatively,
non-conducting plastic screws may be used.
Gas inlet and anode structure may be supported by means of an
annular plate 39 disposed in the central aperture of endwall
portion 14 as by engagement of outwardly projecting flange portion
41, thereof, with inwardly projecting lip portion 42 of endwall
portion 14. An insulating gasket 43 or plastic (Nylon) screws (not
shown) may be used to secure such members in insulated sealed
relation. A tubular conduit section 44 may be secured as by brazing
to the periphery of the central aperture in plate 39 and extending
outwardly therefrom. A cup-shaped hollow anode 46, e.g., of copper
is disposed in coaxial relation in conduit section 44 and may be
supported by an insulating seal means 47 situated between the outer
ends of the conduit and anode. While a cup-shaped anode is shown,
and is preferred for maximum output, it may be noted that a water
cooled-cylindrical or circular plate anode mounted similarly may be
used and often yields a more uniformly distributed output. The
inward end surface of such an anode may terminate about flush with
the inner surfaces of the endwall portions. An insulating sleeve
such as a silica sleeve 48 is disposed in loose fitting relation in
the space between the conduit section 44 and the anode 48 to
minimize arcing therebetween. With button and disc type anodes a
conduit 49a may communicate with the space between the conduit and
anode for directing a puff of an appropriate gas to flow
therethrough and emerge about the periphery of the anode. However,
with a hollow anode 46, it is preferred that a conduit 49b be used
instead to direct the gas through the central hollow portion
thereof. The puffer stream of gas may be supplied from a gas source
reservoir 51 through a needle or similar valve 52 as controlled by
a solenoid valve 53. Gases such as hydrogen, deuterium,
deuterium-tritium mixtures may be used as required in fusion
reactor practice.
A low voltage D. C. power supply means 54, providing rectified and
filtered current, may be connected, as by means of conductors 56,
57 to plate onductors 27, 33 to supply energizing current to
filaments 21. A pulse power supply 56 with the negative terminal
connected to the negative terminal of the filament supply as well
as to conductor 57 and with the positive terminal connected through
conductor 58 to a terminal post 59 attached to anode 46, may be
used to establish the electron arc discharge in chamber 12. High
amperage at a few hundred volts, e.g., 300 volts usually suffices
for such purpose. To minimize the tendency of the gas to pass
through the chamber with too short a transit time, a deflector
plate or hat 61 may be positioned outwardly from anode 46 as by
means of a rod 62 attached thereto.
At the open end of the discharge chamber 12 an annular plate member
63 is provided as a support or mounting means. Member 63 may be
mounted by means of a flange 64 on wall portion 13 through which
screws 66 pass but which are insulated therefrom by a washer 67 and
sleeve 68. The screws 66 engage threaded portions of plate member
63 while an insulating gasket seal 69 is disposed between flange
64, the end of wall portion 13 and a recessed portion of member 63.
The central opening therein defines an ion extraction port.
As employed for injecting energetic particles into a fusion reactor
the foregoing arrangement is provided with an extractor arranged
outwardly of the open end of the discharge chamber. To accommodate
a conventional accel-decel extractor arrangement, an extension of
the vessel 11 may be provided as a cylindrical tubular section 71
having at one end a flange 72 attached in sealed insulated relation
to flange as by means of non-conductor machine screws 73. A flange
74 at the opposite end may be used to attach the plasma source to
an injector port of a controlled fusion reactor, for example, the
2XII, Baseball II or any other appropriate reactor. When so
connected the source is evacuated by the vacuum pumping equipment
of the fusion reactor. Insulators 74 mounted on the inner walls of
tubular 71 may serve to support the grid elements of the
accel-decel system which grids may comprise plates provided with
matching slots or apertures usually circular. More specifically, a
first accel-grid 76 is disposed transversely across the extraction
channel which extends through section 71 facing the plasma in
discharge chamber 12 while a decel grid 77 is disposed thereafter
in spaced-parallel, matching-orifice relation. A third grid 78 is
disposed in similar relation to grid 77 at the outlet of section
71. A particularly effective accel-decel grid geometry is disclosed
in Report UCRL-72880 referenced in Nuclear Science Abstracts 25
38451, Aug. 31, 1971. Electrical potentials for energizing the
extractor may be supplied from a pulsed D.C. power supply 71. Power
supply 71 delivers a potential, V.sub.1, through a conductor 81,
through a sealed feedthrough insulator (not shown) to grid 76.
Similarly, a second potential, V.sub.2, is delivered through
conductor 82, to grid 77 and a third potential, V.sub.3, to grid
78. Potential, V.sub.1, is generally a high positive potential,
e.g., 22 kilovolts and, V.sub.2, a negative potential, e.g., -2
kilovolts (may be varied, e.g., 1 to 4 kilovolts) to repel
electrons from the extracted beam. Potential, V.sub.3, may then be
20 kilovolts which yields a beam of 20 kilovolt particles.
In typical operating cycle a timing sequence may comprise turning
filaments power on at -4 seconds, i.e., for a few seconds adequate
to reach emission temperature; pulsing gas at -20 milliseconds;
applying arc power at t=o; and turning arc power off at t=+15
milliseconds (or other period as desired).
With such a pulsing technique overheating of the components is
minimized despite the large input energies which are used. Cooling
water coils (not shown) may be attached as by brazing to various of
the external surfaces of the various vessel components and exposed
end of the anode to cool the source more rapidly. Insulating
varnish may be applied to interior vessel surfaces or insulation
such as mica used to minimize undesired arcing. Also, a solenoid,
circumjacent vessel section 13 and capable of generating a low
intensity magnetic field, e.g., up to 20 Gauss in chamber 12 may
assist in normalizing arc current across extraction port.
In the ion or plasma source using the described geometry including
a small anode a relatively high electron current ionising
efficiency is obtained so that relatively large gas flows can be
ionized, e.g., to provide ion currents of at least about
1A/cm.sup.2 at the extraction port. For example, a 20A beam may
correspond to a gas flow rate of about 300 cm.sup.3 /min (STP) or
3,600 .mu.1/sec. The ion current has a uniformity within about 15
percent to as low as 5 percent of the mean as measured by means of
a traversing probe (not shown) and with a tungsten screen disposed
across the extraction port to simulate the extractor.
It may be noted that due to the high gas density employed in the
system a very substantial rate of charge exchange occurs. This
effect also occurs in the channels which communicate between the
plasma source and interior of the reactor chamber. As a consequence
the energetic particle beam which emerges may comprise at least
about 50 percent energetic neutrals, e.g., D, which with an
effective extraction potential of 20 Kv has an energy of 20 Kev.
Such particles are of sufficient energy to produce a substantial
fusion rate when trapped to produce a plasma of adequate density.
The efficiency of charge exchange neutralization can therefor be
increased by providing a channel of adequate length or augmented by
using a conventional gaseous charge exchange cell at the output of
the source.
With the 2XII experimental device mentioned above the present
source would be mounted to direct the neutral particle beam
transversely through the containment zone just after the normal
plasma has been trapped to augment the plasma density therein (c.f.
Application Ser. No. 53,056(70) of F. H. Coensgen et al., filed
July 8, 1970).
EXAMPLE
Arc discharge chamber diameter 9 inches Arch discharge chamber
length 2 inches Filament perimeter diameter 81/4 inches Filament
length in chamber 13/4 inches Filaments 0.020 inch thickness
tungsten wire hairpin 26 only Filament current 25A each (approx
1800 amp.) Arc/current (35-60 volts) Approx 600-1200 amp. Pulse
length 5-100 millisec. Anode diameter O.D. circular plate 5 inch.
Accel potential (V.sub.1) +22 Kv Decel potential (V.sub.2) (-1 to
-4Kv) -2 Kv (Net accel potential) (V.sub.3) +20 Kv Ion Current
0.5-1am/cm.sup.2
While there has been described in the foregoing what may be
considered to be preferred embodiments of the invention,
modifications may be made therein without departing from the
teachings of the invention and it is intended to cover all such as
fall within the scope of the appended claims.
* * * * *