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| United States Patent | 4645973 |
| Link to this page | http://www.wikipatents.com/4645973.html |
| Inventor(s) | Salinier; Guy (Paris, FR);
Bossard; Jean-Paul (Fontenay-le-Fleury, FR) |
| Abstract | The hyperfrequency energy is conveyed through a waveguide (1) having a
rectangular section. A central plasmagenic gas and an annular sheathing
gas are supplied through a T-shaped transverse pipe (2). The upper
branches of the T extend in a sealed manner through the small sides of the
waveguide. The stem of the T extends with clearance through an opening (7)
formed in a large side of the waveguide and is provided with a nozzle (22)
which is surrounded by a sleeve (3) terminating in a rolled-over flange
(25). Application in the treatment of surfaces and the production of
chemical reactions. |
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Title Information  |
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Drawing from US Patent 4645973 |
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Hyperfrequency energy plasma torch |
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| Publication Date |
February 24, 1987 |
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| Filing Date |
October 2, 1984 |
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| Priority Data |
Oct 03, 1983[FR]83 15713 |
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Title Information  |
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Claims  |
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What is claimed is:
1. A microwave plasma torch for creating a plasma jet, comprising: a
waveguide for connection to a microwave generator, said waveguide having
lateral walls and defining an opening in a first said wall and a lateral
orifice in a second said wall adjacent said first wall; a gas supply
conduit in the waveguide, the gas supply conduit having a generally
T-shape defining a stem, a first upper branch and a second upper branch;
said stem of said supply conduit constituting a downstream part of said
supply conduit which extends through said opening with clearance and has
an open outlet end and is connected to a discharge nozzle, said first
upper branch extending on a first side of said stem, through said lateral
orifice without clearance and being adapted to be connected to a source of
said gas, and said second upper branch being in alignment with said first
branch, on a second side of said stem opposite to said first side, and
extending to an end portion adjacent a third said lateral wall of said
waveguide which is opposed to said second wall; and means closing said end
portion of said second upper branch.
2. A plasma torch according to claim 1, wherein said waveguide has a
rectangular section and said stem and upper branches are rectilinear and
perpendicular to the respective walls of the waveguide.
3. A plasma torch according to claim 2, wherein said first wall forms a
large side of said waveguide.
4. A plasma torch according to claim 1, further comprising a central
conduit disposed in said stem of said gas supply conduit and a second gas
supply conduit connected to said central conduit.
5. A plasma torch according to claim 4, wherein said second gas supply
conduit is disposed coaxially in one of said upper branches and an elbow
connects said second gas supply conduit to said central conduit.
6. A plasma torch according to claim 5, wherein said second gas supply
conduit is disposed coaxially with respect to said second upper branch and
extends through said third wall.
7. A plasma torch according to claim 4, wherein said nozzle has an exterior
cap of a dielectric material.
8. A plasma torch according to claim 1, wherein said stem of said gas
supply conduit is surrounded by a sleeve having an inside diameter which
is substantially equal to a diameter of said opening, said sleeve being
fixed to said waveguide around said opening.
9. A plasma torch according to claim 8, comprising an outer rolled-over
flange on a downstream end of said sleeve.
10. A plasma torch according to claim 8, comprising an outer bead having a
rounded contour on a downstream end of said sleeve.
11. A plasma torch according to claim 6, wherein said second gas supply
conduit extends through said closing means. |
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Claims  |
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Description  |
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The present invention relates to a plasma torch of the type comprising a
waveguide adapted to be connected to a microwave generator, and a gas
supply conduit which has a downstream part which extends through an
opening of the waveguide with clearance and is connected to a nozzle.
Torches of this type, which have been recently proposed, provide at the
outlet of the pipe a stable plasma in a central plasmagenic gas stream,
which may be sheathed by an annular stream of another gas, or in an
annular stream of plasmagenic gas which may surround a central stream of
another gas. However, these known torches have not permitted reaching
sufficient power to envisage their use in industry.
An object of the invention is to provide a plasma torch which is simple in
construction and is capable of satisfying this need.
The invention therefore provides a plasma torch of the aforementioned type,
wherein the supply conduit has a generally T-shape whose stem constitutes
said downstream part, a first upper branch of the T extending without
clearance through a lateral orifice of the waveguide and being adapted to
be connected to a source of gas, while the second upper branch of the T
extends to the lateral wall of the waveguide opposite said orifice and is
closed.
In an embodiment which still further increases the power of the torch and
enables the latter to be used in a large number of various applications,
in the downstream part of the conduit there is disposed a central conduit
connected to a conduit supplying a second gas, this supply conduit being
disposed coaxially in one of the upper branches of the T and being
connected to the central conduit by an elbow.
One embodiment of the invention will now be described with reference to the
accompanying drawings, in which:
FIG. 1 is a sectional view of a plasma torch according to the invention
taken along line I--I of FIG. 2;
FIG. 2 is a sectional view taken along line II--II of FIG. 1.
The plasma torch shown in the drawings comprises mainly a waveguide 1, a
gas supply pipe 2 and a sleeve 3, all these elements being of metal.
The waveguide 1 is rectilinear and has a rectangular section shown in FIG.
2. It extends from a microwave generator (not shown and located at the
left as viewed in FIG. 1) to an end which is closed by a quarter-wavetrap
4 which is adjustable in position by a slidable rod 5 which extends out of
the end of the waveguide. Such traps are well-known in the hyperfrequency
art and need not be described in detail. For convenience of the
description, it will be assumed that the axis X--X of the waveguide is
horizontal as are the large sides of the rectangular section of this
waveguide.
The waveguide 1 includes a removable intermediate section 6 whose lower
side has a circular opening 7 having a vertical axis Y--Y and whose
lateral sides have two circular orfices 8 and 9 respectively. The orifices
8 and 9 have the same diameter less than the diameter of the opening 7 and
are in alignment on a common horizontal axis Z--Z. The axes X--X, Y--Y and
Z--Z intersect at the centre of the section of the waveguide located in
the plane of symmetry of the section 6.
The supply pipe 2 is adapted to convey two different gases respectively
through an exterior conduit 10 and an interior conduit 11.
The exterior conduit 10 has a generally T-shape. An upper branch 12 of the
T, having an axis Z--Z, extends through the orifice 8 in a sealed manner
and terminates in a coupling 13 for connection to a source (not shown) of
a first gas. The other upper branch 14 of the T, which also has an axis
Z--Z, has its end portion fitted in a sealed manner in the orifice 9 and
is hermetically closed by a washer 15. The stem 16 of the T extends
coaxially through the opening 7 with a large clearance.
The interior conduit 11, provided with a coupling 17 for connection to a
source (not shown) of a second gas, comprises an upstream part 18 having
the axis Z--Z and extending through the washer 15 in a sealed manner, an
elbow 20, and a downstream part 21 having the axis Y--Y. The part 21
includes a collar which is axially apertured so that it is centered in the
stem 16 of the T and allows the passage of the first gas.
The whole of the pipe 2 can consist, as shown, of a succession of tubular
elements which are screwed together, fluidtightness being preferably
achieved by welds. Screwed on the lower end of the stem 16 is a nozzle 22
having a conical nose of conventional type in oxygen cutting, a central
conduit of which communicates with the conduit 11 while an annular conduit
(or a series or conduits disposed in a ring arrangement) communicates with
the conduit 10. The nozzle 22 bears against an interior shoulder 23 of the
conduit 10, with interposition of a suitable sealing element (not shown),
and is held in position by a nut 24 screwed into this conduit.
The sleeve 3 has an inside diameter substantially equal to the diameter of
the opening 7. It has at its upper end an outer flange 24 screwed in
position around this opening and, at its lower end, a rolled-over flange
25. This flange, which is connected tangentially to the cylindrical wall
of the sleeve, can have a contour in the shape of an arc of a circle, as
shown. By way of a modification, this flange 25 may be replaced by an
outer bead which has a rounded contour and is tangentially connected to
the sleeve. The lowermost circle of the flange 25 or bead is substantially
in the horizontal end plane of the nozzle 22.
In operation, one of the two couplings 13 and 17 is connected to a source
of a plasmagenic gas, for example argon, and the other is connected to a
source of another gas adapted to sheath the plasmagenic gas or to be
surrounded by the latter at the outlet of the nozzle 22. The microwave
generator supplies a pulsating electromagnetic energy, for example at the
frequency of 2.45 GHz.
The incident power is divided into a useful power transmitted by the pipe 2
and the nozzle 22 which consititutes an antenna in the absence of gas, and
a parasitic reflected power returned by the waveguide 1 to the generator.
The applicant has found that, surprisingly, with a suitable adjustment of
the trap 4, it was possible to obtain a stable plasma at the outlet of the
nozzle 22 with an efficiency, useful power/incident power, on the order of
95% for an incident power ranging up to at least 6 kW. Satisfactory tests
have in particular been carried out with a central argon plasma sheathed
with compressed air or nitrogen. By eliminating the gas sheath, it was
possible to obtain a stable plasma up to an incident power of about 4 kW.
By way of a modification, the exterior cap of the nozzle may be made from a
dielectric material (quartz, ceramic, etc.). This permits increasing the
power of the torch or, for a given power, reducing the required gas flows.
Further, if the torch is intended to operate under conditions which are
always identical, the trap 4 may be replaced by a simple planar plate
having an axis X--X and connected hermetically to the waveguide.
In another modification, when the conduit 11 conveys a plasmagenic gas,
there may be introduced through the branch 12 of the T a gas mixture, for
example a combustible mixture, so as to form at the outlet of the nozzle
22 a flame sheathing the central plasma jet. In this case, it may be
advantageous, for reasons of safety, to arrange that the gases of the
mixture (for example O.sub.2 and H.sub.2) be conveyed separately up to the
outlet of the nozzle 22 and mixed only outside the latter, as is usual
with certain types of burners. Suitable pipes and/or partition walls are
then provided in the branch 12 and in the stem 16 of the T.
The torch described above may in particular be employed for the treatment
of surfaces, for producing chemical reactions or for scientific
applications such as analysis operations.
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Description  |
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