Plasma torch with a microwave transmitter

Information

  • Patent Grant
  • 6388225
  • Patent Number
    6,388,225
  • Date Filed
    Monday, October 2, 2000
    26 years ago
  • Date Issued
    Tuesday, May 14, 2002
    24 years ago
Abstract
A plasma torch with a microwave transmitter which, for example, is used to coat surfaces and to produce radicals. The plasma torch exhibits a minimal energy loss during the transmission of microwaves to the produced plasma flame. The plasma torch includes a waveguide for transmitted microwaves and has a coaxial conductor. An electrode is provided with a duct, and a nozzle provided on the other end of the duct, the end facing away from the waveguide, are arranged in the coaxial conductor in an essentially axial manner. The plasma flame is produced at the nozzle. A coupling element is arranged between the waveguide and the coaxial conductor. The electrode is connected to the coupling element via a mounting plate and an electrically insulating intermediate element in a gas tight, thermally insulated manner such that microwaves are permitted to pass through.
Description




SPECIFICATION




The invention relates to a plasma torch with a microwave transmitter, according to the kind of patent claims which, for example, is used to coat surfaces and to produce radicals.




Known magnetron-ion sources employ a magnetron for generating an alternating electric field; refer to DE 37 38 352 A1. It is an disadvantage that a quartz dome and external magnetic fields are required to generate the gas plasma. The intensive magnetic field in the discharge chamber is used to match the cyclotron frequency to that of the microwave generator. The operation of the microwave gas discharge takes place without electrodes. Furthermore, the operation requires a cooling of the device. Such plasma generators are of a complex structure and are limited in their dimensions. The technical expenditures for microwave gas discharges systems are high. It is not feasible to transmit high powers, and it is not evident that plasmas of high density are stable when high powers are concerned.




Devices for generating plasmas by microwaves, as known from, for example, DE 3905303 C2, DE 3915477 C2. U.S. Pat. No. 5,349,154 A, generally use quartz tubes. A magnetron (microwave transmitter unit) is secured to one end of a rectangular hollow guide. The generated microwaves pass through the hollow guide and impinge, at the other end of the hollow guide, upon a quartz glass insert through which a special gas flows. The flowing originates from a low pressure maintained in the recipient. In the quartz glass insert a plasma is generated by the microwave energy, and the plasma flows through the quartz glass insert into the recipient. The method is characterized by not having any electrodes. Such devices exhibit the following disadvantages:




The hottest site and the center of the plasma are located in that portion of the quartz glass insert, which is arranged within the rectangular hollow guide. Hence, the energy is transformed before the recipient rather than within the same and, at a respective application, too little radicals are provided for the operation process.




A high rate of wall effects occur within the quartz glass.




The mass throughput and the effective pressures of 500 Pa to 3 kPa are too low.




The quartz glass insert is not suited for any large-scale technical continuous operation. Due to the unintentional high temperatures the quartz glass insert shows melting effects, or there have to be additionally provided expensive cooling devices.




The efficiency of the energy exploitation is low.




It is difficult to maintain the vacuum tightness at the sealing faces.




In the course of mounting and dismounting, respectively, and due to the thermal expansion of the metallic components it can be possible that the glass will be destroyed.




Furthermore, devices are known, in which a cross-coupling of a rectangular hollow guide with a coaxial guide is provided. Also in this case, a microwave generating device and a microwave transmitter device, respectively, i.e. a magnetron, are secured to one end of a hollow guide. The generated microwaves pass through the hollow guide and impinge upon a conductive longitudinally extending nozzle. The hollow guide is closed by a short-circuit slide. In this way, the resulting electromagnetic wave is tunable. Such a known arrangement can be designed with a quartz tube (DE 195 11 915 C2) or without one (U.S. Pat. No. 4,611,108 A). Apart from the fact that when using quartz tubes the specific disadvantages occur as mentioned above, this cross-coupling features the following disadvantages:




The exploitation of the microwave output is of low efficiency.




Energy losses occur at the cross-coupling between the rectangular hollow guide and the coaxial guide.




The entire construction is complicated.




The maximal operation pressure and the mass throughput are too little.




From U.S. Pat. No. 4,473,736 A a plasma generator is known, in which a cavity and a coaxial guide are capacitively coupled. Insulating thin disks supporting the electrode are arranged distributed along the entire cross-section of the cavity and the coaxial guide. Apart from not being a hollow wave guide, this arrangement is not suited for an impedance matching and for obtaining a low-reflective hollow wave conduction.




Hence, it is an object of the present invention to provide a plasma torch that generates plasma with high densities in a range near normal pressure. Thereby high powers are capable to be transmitted. A stable combustion and an efficient exploitation of the microwave energy shall be a feature of the plasma torch. Susceptible quartz tubes or quartz domes for generating plasmas have to be avoided. There is a plasma torch aimed at, which is simple in its entire setup.




According to the invention the object is realized by the features of the Patent claim. As a matter of fact, it is initially irrelevant whether or not the coaxial guide is, in a cross-coupling, directed transversally to the hollow guide or, in an axial coupling, in parallel to the hollow guide, whether consequently their longitudinal axes preferably include a right angle or whether or not their longitudinal axes substantially coincide. The plasma torch (plasma generator) comprises a vacuum chamber and a magnetron, which within the vacuum chamber generates itself a field intensity sufficient for plasma formation. A recipient succeeding the coaxial guide is under a pressure of 100 Pa to 10 kPa, this pressure is suited for the formation of a plasma. A high efficiency is attained irrespective of the kind of coupling. The inventional plasma torch does without a cooling and without magnet coils due to its simple axial setup with an antenna as an electrode. The advantage in using a hollow wave guide instead of an a. c.-waveguide lies in the fact that the microwave output is not only coupled in the plasma in the vicinity of the nozzle, where there are the highest field intensities, but via the hollow space waves along the entire hollow guide axis. Such a design permits a quasi-electrodeless coupling-in that reduces the thermal stress of the nozzle. Advantageously, the hollow electrode is designed as a truncated cone and secured to a non-conductive intermediate member that is connected to the coaxial guide via a preferably disk-shaped mount. The nozzle is connected to a gas inlet through this intermediate member. The mounting disk is flanged to the coaxial guide and to the hollow guide. Advantageously, the hollow electrode is designed as a truncated cone, the shell of which is in opposition to the recipient. The hollow electrode is provided with an exchangeable nozzle that is inserted, preferably screwed into the inside space; the nozzle comprises four exit orifices for the operation gas, the exit orifices are arranged in the exit plane, regularly spaced from each other on a circle centered about the exit plane. In this way, an optimal directing of the microwave to the exit plane (nozzle tip) is achieved and a favorable energy input into the plasma flame is attained. A nozzle adapted for high temperatures preferably consists of a metal-ceramic alloy. An electrically non-conductive insulator thermally insulates the space of the plasma flame from the coupling site. An advantageous solution for the operation of the plasma torch is obtained in rendering the electrode axially and, if necessary, radially adjustable. In the case of cross-couplings, a brass member and a second intermediate member preferably connect the nozzle and the first intermediate member to a gas inlet. The brass member in any case ensures the electromagnetic coupling of the hollow conductor and coaxial guide. The hollow guide, preferably a rectangular hollow guide, of the cross-coupling is provided with two screws for tuning the electromagnetic wave to the coupling. In the case of the hollow guide, preferably a round hollow guide, of the axial coupling, the tuning is advantageously carried out in that its length is variable. To this end the hollow guide consists of, for example, two parts that can be telescope like slid one into the other, also during operation. One of the tubes can be provided with longitudinal slots and in-between remaining resilient lugs. A microwave seal is advantageously provided in an annular groove located between the tubes in an overlapping range. At the transition from the coaxial guide to the recipient a vacuum passageway for the electrode and the operation gas is provided; in this way an efficient coupling of the electromagnetic wave is obtained.











In the following, the invention will be explained in more detail by two schematical drawings illustrating two embodiments. There is shown in:





FIG. 1

a longitudinal cross section of a cross-coupling of a rectangular hollow guide with a coaxial guide;





FIG. 2

a longitudinal cross section of an axial coupling of a round hollow guide with a coaxial guide;





FIG. 3

an enlarged representation of a front view of the nozzle.











In

FIG. 1

, a cylindrical coaxial guide


2


having a longitudinal axis Y—Y is coupled by a coupling member


3


in the vicinity of one of its ends to a rectangular hollow guide


1


with a longitudinal axis X—X in such a way that the longitudinal axis X—X and Y—Y are at right angles to each other. The coupling member


3


is designed like a bowl with a central opening


4


and a circumferential flange


5


and contains a disk


6


for engaging an intermediate member


7


made of insulating material. By way of a ring


8


screwed to the circumferential flange


5


, the disk


6


is rigidly and tightly connected to the coupling member


3


. The central opening


4


in the coupling member


3


corresponds to a same opening


9


in the rectangular hollow guide


1


. This opening is also surrounded by a flange


10


, to which the coupling member


3


is screwed on tightly. The ring


8


is the end-portion of a hollow conductor


20


that comprises an insulator


11


at the other end of which a recipient


12


is provided. The mounting disk


6


, the intermediate member


7


, and the insulator


11


are designed strong enough and form together a gas-tight, thermally insulating crossover, however permitting passage of microwaves, between the rectangular hollow guide


1


and the hollow conductor


20


. The intermediate member


7


additionally must have dielectric properties that ensure a low-reflection waveguiding at the crossover.




A cone-shaped electrode


13


made of a metal-ceramic alloy is secured to that side of the intermediate member


7


facing the recipient


12


. The electrode


13


, as is the intermediate member


7


, is provided with an axial passageway


14


into which at the free end of the electrode


13


a nozzle


22


is secured or exchangeably inserted, preferably by screwing. The longitudinal axis of the electrode


13


coincides with the axis Y—Y. On the other side of the intermediate member


7


, a brass member


16


, which is provided with an axial bore


15


, is connected to the passageway


14


; an insulating connecting member


17


in continuation of the axial bore


15


is attached to the brass member


16


and leads to a gas inlet


18


. The connecting member


17


is supported by a flat mount


19


which is tightly screwed to the rectangular hollow guide


1


. The cylindrical hollow conductor


20


and the electrode


13


together form a coaxial guide


2


. The electrode


13


, which is in the shape of a truncated cone, is positioned in a respective recess


21


of the insulator


11


in such a way that the nozzle


22


projects beyond the insulator


11


on the side of the recipient.




The rectangular hollow guide


1


is provided with a magnetron


23


at its other end, the magnetron generates microwaves, which are transmitted through the guide


1


. Two screws (steps)


24


are provided for affecting microwaves for the coupling. The microwaves generated by the magnetron


23


pass through the guide


1


and are tuned by the screws


24


to the coupling. By way of the cross-coupling a longitudinal wave is coupled out into the coaxial guide


2


so that an axial electromagnetic field results. The cross-coupling consists of a coupling rod that is substantially identical to the electrode


13


, with which the coupling rod projects into the round hollow conductor


20


, both together form the coaxial guide. The coupling rod


13


has the task to direct the operation gas and to assist in generating a plasma and a plasma torch


25


, respectively, at the orifice of the nozzle


22


. The gas supply into the coupling rod is provided from the external gas inlet


18


via the bores


15


in the connecting member


17


made of teflon and in the brass member


16


, and via the passageway


14


of the intermediate member


7


, which is also made of teflon. The brass member


16


also ensures a good coupling of the microwave. The electrode


13


is secured in and insulated against the coaxial guide


2


by the connecting member


7


. The geometry of the electrode


13


is optimally adapted to the requirements of the procedure. It ensures a maximal dielectric strength. Its favorable length is important for its operation, which length can be varied by adjusting the passageway


14


by way of the thread in the electrode


13


. Its cross-section is so selected that the coaxial guide


2


ensures an optimal guiding of the electromagnetic wave and that the highest field strength is obtained at the tip of the nozzle. This is very important since the plasma is ignited at the site of the greatest field strength. The nozzle


22


is made of a special material. It consists of a compound material, which has ceramic components and is metallically conductive. The task of the ceramics is to thermally insulate the plasma cloud from the electrode


13


. The plasma is operable up to a pressure of 35 kPa. A considerably greater mass throughput can be obtained by that. This is a great advantage since considerably more co-reactants can be generated in a respective process. Thus it is feasible to strongly reduce the process times due to the considerably increased mass throughput. A further advantage of such a burner lies in the fact that these parameters can also be obtained with air as a process gas. Thus, one can do without expensive additional gases such as, for example, noble gases (argon).




In

FIG. 2

an air-cooled magnetron


23


connected to a control device


26


is mounted on a base plate


30


together with a fan


27


, a thermo-regulator


28


, and a heating-current transformer


29


. The magnetron


23


for generating the microwaves has an output of 2 kW and emits electromagnetic waves at a stable frequency of 2.45 GHz and a wavelength of 12.24 cm. Its output can be linearly controlled by the control device


26


between 10% and 100% of the maximal power. The thermo-regulator with a thermal circuit-breaker is connected to the resonator of the magnetron


23


. At a temperature of 120° C. the thermo-regulator turns OFF the magnetron for safety reasons.




The base plate


30


is secured to a round hollow guide


31


that comprises an internal tube


32


which has a diameter of 100 mm and a wall thickness of 2 mm, and an external tube


33


which has a diameter of 104 mm and a wall thickness of 2 mm. The tubes


32


,


33


are well-fitted one into the other and can be, telescope-like, mutually and slidingly displaced. They can be mutually fixed by a clamping screw


34


. The external tube


33


is provided with longitudinal slots


35


(only one visible) in order to create a certain squeezing when the tubes are displaced, so that resilient lugs at the external tube


33


result between the slots


35


which slightly press against the interior tube, thus substantially preventing an unintentional mutual displacement of the two tubes


32


,


33


even when the clamping is released. Simultaneously, the electrical contact between the tubes


32


,


33


is improved thereby, and flash-overs between the tubes are avoided. In order to ensure a microwave sealing of the round hollow guide


31


, a microwave seal


36


, for example, in the form of a metallic gauze, can be inserted into the annular groove between the two tubes


32


,


33


. The external tube


33


is provided with a flange


37


at that of its ends facing away from the magnetron


23


. This flange


37


provides for an axial coupling to a following coaxial guide


2


which has a common longitudinal axis X-Y with the round hollow guide


31


. This coupling provides for coupling out of a longitudinal wave into the coaxial guide


2


, and an axial electrical field results.




The coaxial guide


2


, as well as the subsequent recipient


12


attached thereto, have the same diameter and cross-section, respectively, as the external tube


33


. Thereby, the recipient


12


simultaneously fulfills the task of a hollow guide that prevents a lateral propagation of the waves, and in this way couples-in the microwave power into the plasma


25


over a considerable path behind the nozzle


22


along the axis X-Y (also along the axis Y—Y in FIG.


1


). The coaxial guide


2


has also a flange


38


at its end which is facing the round hollow guide


31


. This flange


38


matches the flange


37


and is screwed to the latter and forms with the latter a coupling member which corresponds to the coupling member


3


in FIG.


1


. Both flanges


37


,


38


encompass the circumference of an engaging disk made of any desired material (aluminium, quartz glass) and hermetically and firmly support the disk. The interior conductor


39


of the coaxial guide


2


is suspended electrically insulated in this disk


6


via an intermediate member


7


made of PTFE. The use of Teflon has the advantage that it is easily workable and that it ensures a permanent vacuum tightness. Furthermore, this vacuum passageway fulfills the task of passing the microwave on to the recipient


12


and of a thermal insulation of the hollow guide


32


from the hot plasma


25


. The interior conductor


39


provides for the coupling of the round hollow guide and the recipient, for the supplying gas, and for the expansion of the gas into the recipient


12


via a nozzle


22


screwed into an electrode


13


. In order to tune the microwave, the position of the interior conductor


39


in the coaxial guide


2


and its length are adjustable. The electrode


13


is secured to the intermediate member


7


and, as the latter does, has a passageway (


14


) for the gas supply. A compressed-air hose


40


made of PE (polyethylene) can be connected to this passageway


14


via a brass member (similar to that in FIG.


1


). The intermediate member


7


, the electrode


13


, and the nozzle


22


form an antenna, the outer diameter of which is 20 mm. The longitudinal axis of the antenna coincides with the axis X-Y. The plasma


25


ignites at the nozzle


22


screwed into the end of the antenna. A detachable connection between the electrode


13


and the nozzle


22


is important, to enable exchange or renewal of the nozzle


22


. Since the nozzle is exposed to very high thermal loads it is made of highly heat-resistant steel; for example, a metallic alloy is used having a maximal operation temperature of 1425° C. This material is characterized in that the nozzle


22


is metallic conductive and forms a ceramic surface under the influence of high temperatures that can resist the high temperatures. Since the frequency of the microwaves used lies below the plasma frequency, it can not propagate within the plasma


25


. Hence, in order to realize as good as possible an energy input into the plasma


25


, the surface of the plasma cloud has to take a maximum. Therefore, the nozzle


22


provides for a strong vorticity of the plasma


25


. To this end and according to

FIG. 3

, four abaxial gas exit orifices


43


are provided in the exit plane


41


of the nozzle


22


, in a preferably regular arrangement on a circle


42


, each of the gas exit orifices having a diameter of 1 mm. In order to thermally insulate the plasma flame from the flanges


38


,


39


and from the disk-shaped mount


6


, respectively, a thermal insulator


11


is arranged between the disk-shaped mount


6


and the plasma torch


25


, the electrode


13


and the nozzle


22


projecting through the thermal insulator


11


. Just as the coaxial guide


2


, the recipient


12


consists of a tube with a diameter of 104 mm, a wall thickness of 2 mm and a length of 300 mm. It can be provided with not shown means for temperature measurement, for pumping off, and for observing the flame. Advantageously, air is used as an operation gas. The operation of the plasma


25


is possible up to a pressure of 100 kPa. With that still a greater mass throughput can be obtained. The inventional axial coupling is particularly well suited to generate as high as possible an energy in the recipient and many radicals.




In total, the inventional axial coupling offers the following advantages:




It enables an efficient exploitation of the microwave power.




It permits an uncomplicated setup.




It ensures a high maximal operation pressure and mass throughput.




It eliminates the energy losses inherent in the cross-coupling.




The mutual fixation of the tubes


32


,


33


can be achieved by using a clamping ring encompassing both tubes instead of using the clamping screw


34


. For performing length variations of the round hollow guide


31


, also a membrane bellow and exchangeable round hollow guide members can be used. It is advantageous for a fast, simple and precise adjustment of the length of the round hollow guide to be capable of adjusting the membrane bellow in steps or continuously also during operation of the inventional device along a linear guide.




All features disclosed in the specification, in the subsequent claims, and in the drawing can be substantial for the invention both, individually and in any combination with one another.















List of reference numerals


























 1




rectangular hollow guide







 2




coaxial guide







 3




coupling member







 4, 9




openings







 5, 10, 37, 38




flanges







 6




mounting disk (disk-shaped mount)







 7




intermediate member







 8




ring







11




insulator







12




recipient







13




electrode (coupling rod)







14




passageway







15




axial bore







16




brass member







17




connecting member







18




gas inlet







19




mount







20




hollow conductor







21




recess







22




nozzle







23




magnetron







24




screws (steps)







25




plasma







26




control device







27




fan







28




thermo-regulator







29




heating-current transformer







30




base plate







31




round hollow guide







32




interior tube (inner tube)







33




external tube (outer tube)







34




clamping screw







35




(longitudinal) slot







36




microwave seal







39




interior conductor







40




compressed-air hose







41




exit plane of nozzle







42




circle







43




gas exit orifices







X-X; Y-Y; X-Y




(longitudinal) axes














Claims
  • 1. A plasma torch comprising:a microwave transmitter for emitting microwaves; a hollow guide for guiding the emitted microwaves; a coaxial guide; an electrode including a passageway; a nozzle on the electrode at that end of the passageway facing away from the hollow guide; said electrode and said nozzle being arranged in a substantially axial manner in said coaxial guide, whereby a plasma cloud is produced at the nozzle, said plasma cloud being directed towards a recipient; a disk-shaped mount; a coupling member coupling the hollow guide and the coaxial guide and gas tightly supporting the disk-shaped mount; an electrically and thermally insulating intermediate member include a passageway and being arranged in the disk-shaped mount; and said electrode, on a side opposite the hollow guide, being connected gas-tightly, but transmissive to microwaves, to the electrically and thermally insulating intermediate member.
  • 2. A plasma torch as claimed in claim 1, wherein said electrode is designed as a truncated cone.
  • 3. A plasma torch as claimed in claim 2, wherein said nozzle and said electrode are adjustable in parallel and at right angles to the longitudinal axis of said hollow guide.
  • 4. A plasma torch as claimed in claim 3, wherein the insulating connection of the electrode with the coupling member has the shape of an intermediate member provided in a variable suspension.
  • 5. A plasma torch as claimed in claim 4, wherein the longitudinal axis of the electrode is transversally directed to the longitudinal axis of the hollow guide.
  • 6. A plasma torch as claimed in claim 5, wherein at least one screw is provided in said hollow guide, said screw being adjustable transversally to the longitudinal axis of said hollow guide for tuning the microwave field.
  • 7. A plasma torch as claimed in claim 1, 4 or 5 wherein the nozzle is provided with gas exit orifices, which are located outside of the nozzle axis.
  • 8. A plasma torch as claimed in claim 4, wherein the longitudinal axis of the electrode is directed in parallel to the common longitudinal axis of the hollow guide and of the coaxial guide.
  • 9. A plasma torch as claimed in claim 5 or 8, wherein a brass member provided with a bore is pre-positioned to that side of said electrode and said intermediate member, which is opposite to said hollow guide, said bore being arranged in the extension of the passageways through said electrode and said intermediate member.
  • 10. A plasma torch as claimed in claim 9, wherein the passageways are connected to a gas inlet via the bores of the brass member and a connecting member.
  • 11. A plasma torch as claimed in claim 6 or 7, wherein a thermal insulator is provided between the plasma cloud and the disk-shaped mount, the nozzle projecting beyond said thermal insulator in direction of said recipient.
  • 12. A plasma torch as claimed in claim 8, wherein said hollow guide is composed of two tubes which are adapted to be telescope-like slid in and adjusted to one another.
  • 13. A plasma torch as claimed in claim 12, wherein one of the two tubes is provided with longitudinal slots along a part of its length.
  • 14. A plasma torch as claimed in claim 12 or 13, wherein a clamping means is provided for arresting the tubes.
  • 15. A plasma torch as claimed in claims 12 or 13, wherein a microwave seal is provided in an annular groove between the two tubes.
  • 16. A plasma torch as claimed in claim 1, wherein said nozzle is exchangeably secured in said passageway.
  • 17. A plasma torch as claimed in claim 1, wherein the nozzle is made of a ceramic-metallic combination.
  • 18. A plasma torch as claimed in claim 1, wherein the recipient is of a same cross-section as the hollow guide for the emitted microwaves and considerably projects beyond the nozzle tip.
Priority Claims (1)
Number Date Country Kind
198 14 812 Apr 1998 DE
PCT Information
Filing Document Filing Date Country Kind
PCT/EP99/02413 WO 00
Publishing Document Publishing Date Country Kind
WO99/52332 10/14/1999 WO A
US Referenced Citations (7)
Number Name Date Kind
3353060 Yamamoto et al. Nov 1967 A
4473736 Bloyet et al. Sep 1984 A
4611108 Leprince et al. Sep 1986 A
4943345 Asmussen et al. Jul 1990 A
5047115 Charlet et al. Sep 1991 A
5349154 Harker et al. Sep 1994 A
5734143 Kawase et al. Mar 1998 A
Foreign Referenced Citations (6)
Number Date Country
3738352 May 1989 DE
3905303 Aug 1989 DE
3915477 Nov 1989 DE
19511915 Oct 1996 DE
0104109 Mar 1984 EP
0296921 Dec 1988 EP