EP2613614A1 - Device for generating a plasma stream - Google Patents
Device for generating a plasma stream Download PDFInfo
- Publication number
- EP2613614A1 EP2613614A1 EP13162477.7A EP13162477A EP2613614A1 EP 2613614 A1 EP2613614 A1 EP 2613614A1 EP 13162477 A EP13162477 A EP 13162477A EP 2613614 A1 EP2613614 A1 EP 2613614A1
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- European Patent Office
- Prior art keywords
- housing
- channel
- zone
- electrode
- diameter
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Classifications
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/24—Generating plasma
- H05H1/26—Plasma torches
- H05H1/32—Plasma torches using an arc
- H05H1/34—Details, e.g. electrodes, nozzles
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/24—Generating plasma
- H05H1/26—Plasma torches
- H05H1/32—Plasma torches using an arc
- H05H1/34—Details, e.g. electrodes, nozzles
- H05H1/3494—Means for controlling discharge parameters
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/24—Generating plasma
- H05H1/26—Plasma torches
- H05H1/32—Plasma torches using an arc
Definitions
- the present invention relates to a device for generating a plasma stream having a low temperature and a relatively high power.
- the plasma flow is generated by applying a voltage between a cathode formed of a thoriated tungsten bar and an anode forming the body of the plasma nozzle.
- an argon gas flow circulates in the free space separating the anode and the cathode so as to develop the electric arc formed between these two electrodes to an outlet opening of the nozzle.
- the average temperature of the plasma jet is about 5500 ° K which is still too high for the surface treatment applications contemplated by the present invention.
- the present invention therefore aims at providing a device enabling generate a plasma stream whose temperature is low while having a relatively high power.
- a device for generating a plasma flow comprising an electrically conductive box of tubular form forming a central channel through which a swirling gas passes, a central electrode disposed coaxially in said channel and a electric power source for applying an electrical voltage V between the electrode and the housing, characterized in that the average diameter of the channel formed by the housing decreases progressively from an area substantially at the free end of the housing electrode to an end zone of said housing, said end zone being configured such that the minimum electrical voltage Vcmin (0) to be applied to develop an electric arc between said electrode and said end zone is strictly greater at said voltage V.
- the device according to the invention makes it possible to limit the development of an electric arc inside a conductive casing to an end zone positioned just before the opening of the casing intended to deliver the flow of plasma over the piece to be treated.
- the end zone is configured so as to develop an electric arc with the central electrode only from a certain minimum voltage. Therefore, by applying a voltage lower than said minimum voltage, the electric arc develops inside the central channel of the housing to approach or even reach said end zone, then retracts abruptly in the direction of the central electrode. Subsequently, it resumes its development inside the channel towards said end zone until it retracts again.
- This succession of development and retraction of the electric arc ultimately generates a relatively powerful plasma flow but whose temperature is low enough to allow its use in many surface treatment applications.
- the device 10, represented on the Figure 1 has an electrically conductive box 1 of tubular form, connected to the ground, having an internal cavity joining its two ends, said cavity constituting an elongate central channel 2 within which circulates a swirling gas 3.
- the gas 3 for example air, is introduced into the central channel 2 from an opening 4 formed in the side wall of the housing 1.
- the gas 3 is caused to swirl by means of a swirling device (not shown) so that the gas 3 flows inside the channel 2 forming a vortex substantially helically around the longitudinal axis of the channel 2, coinciding with the longitudinal axis of the housing 1.
- At one end of the housing 1 is mounted an insulating support 6 on which is fixed a central electrode 5 rod-shaped, which penetrates coaxially in the central channel 2.
- An electric high voltage source 7 which can supply a DC voltage, an AC voltage or a pulsed voltage, is connected to the electrode 5 and the earth.
- a device 8 for measuring and regulating the current and the electrical voltage connected between the voltage source 7 and the electrode 5 makes it possible to control the real voltage applied between the electrode 5 and the housing 1.
- the housing 1 formed of a metal and itself connected to earth, serves as a counter electrode so that an electric discharge between the electrode 5 and the housing 1 can be caused. This electric discharge initially occurs in an ignition zone 9, which is in the free space surrounding the electrode 5 and defined by the inner wall of the housing 1.
- the ignition zone 9 will generally be positioned near the the free end of the electrode 5 and downstream of the opening 4 so as to allow the gas 5 to move along the axis of the housing 1 the micro-electric arcs 11 formed at each discharge.
- the micro-arcs 11 lengthen over time along the entire length of the channel 2 and, due to a vortex stabilization of the gas flow towards the axis of the housing 1, form a wire arc
- the end zone 13 may be similar for example to an end channel oriented along the longitudinal axis of the housing end opening on an open end through which the flow of plasma. It may also have a more complex form, as we will see more fully later with reference to Figures 2 to 4 .
- the basic structure of the device 10 as described above does not allow the generation of a low temperature plasma stream. Indeed, in this basic structure, the electric arc 12 is stabilized quickly. The plasma flux is thus generated continuously as long as a voltage V is maintained between the electrode 5 and the housing 1. This operating mode induces the formation of a powerful plasma flux and particularly hot. In addition, in this configuration, the risk is high that the electric arc 12 is formed directly between the electrode 5 and the object to be treated if the latter is metallic. To remedy this, the Applicant has had the idea to limit the development of the electric arc 12, in particular by causing its retraction as soon as it reaches a limit zone inside the housing 1. It turns out that, to maintain sufficient power to the plasma flow, it is advantageous to coincide this boundary zone with the end zone 13 mentioned above.
- a first solution is to first determine the actual voltage Vcmax from which an electric arc is likely to form between the electrode 5 and the end zone 13 of the housing 1.
- Vcmax the actual voltage
- the device 8 is then able to send an interruption signal to the voltage source 7 so as to produce an electrical micro-cut which causes a retraction of the arc 12 to the ignition zone 9.
- the restoration and maintenance of the voltage V again produces the expansion of the arc 12 to the end zone 13 and, therefore, its retraction again.
- an unbalanced plasma stream is generated that is characterized by a relatively low temperature, especially between 30 ° C and 300 ° C.
- a second solution consists in configuring the device for generating the plasma flow such that an automatic retraction of the electric arc 12 occurs when it reaches or approaches the end zone 13.
- This result can notably be obtained by using the particular structure of the housing 1 shown in the Figure 1 .
- the housing 1 has a channel 2 whose section, or the average diameter, decreases progressively from the ignition zone 9 to the end zone 13.
- This progressive decrease may notably consist in segmenting the inner wall of the housing 1 in a series of successive tubular sections S1, S2, S3 and S4 of decreasing diameter and of identical length.
- V is greater than or equal to Vcmin (-1), Vcmin (-1) corresponding to the breakdown voltage of section S3.
- the end zone 13 defines an end channel oriented along the longitudinal axis of the casing 1, said end channel opening on an open end 14 of conical shape through which the plasma flow exits.
- the micro-arcs 11 leave the end channel 13 following the conical surface of said end 14.
- This uniform distribution of the micro-arcs 11 on the surface of the cone ultimately generates a flow of plasma more wide and less intense which allows to further reduce its temperature and allows the device 10 to be used on a wider range of surfaces.
- the end zone 13 defines an end channel oriented along the longitudinal axis of the housing 1, said end channel opening on a channel 15 open at its two ends 16 and forming an angle ⁇ with the longitudinal axis of the housing 1, the angle ⁇ being less than or equal to 90 °. In the configuration shown, this angle ⁇ is substantially equal to 90 °. In this way, the plasma flow F leaves the housing 1 by two openings 16 formed on its side walls and in a direction transverse to the longitudinal axis of the housing 1. This configuration makes it easier to apply the plasma flow F to inside tubes or, more generally, inside hollow objects.
- the device 10 to treat wires 17, or any other filiform object such as tubes or cables, capable of being introduced inside the transverse channel 15.
- wires 17, or any other filiform object such as tubes or cables, capable of being introduced inside the transverse channel 15.
- the wire 17 is in contact with the plasma flow F leaving the end channel 13.
- it will be advantageous to shift the This axis increases the propensity of the plasma flow F to swirl inside the transverse channel 15.
- FIG. Figure 4 there is shown a third possible variant of the end zone that can be used in the device represented in FIG. Figure 1 .
- the end zone 13 defines an end channel oriented along the longitudinal axis of the housing 1, said end channel having a plurality of openings 18 opening on a plurality of transverse channels 19 oriented substantially perpendicular to the longitudinal axis of the housing 1 and one of the ends 20 is open.
- the plasma flow F therefore exits through each of said open ends 20.
- This "comb" distribution of the plasma flow F thus makes it easier to treat wide surfaces.
- the plasma flux exiting the apertures 20 has a variable intensity depending on the position of the apertures 20 in the end channel 13, it may be advantageous to make an additional aperture 21 at the end of the channel. end 13 way partially letting out said plasma stream through said opening 21 and thus uniformize the intensity of the plasma flows leaving the openings 20.
- This example uses the device of the invention in its configuration represented on the Figure 1 .
- Energy source direct current Electrical voltage applied between the electrode and the housing 3 kV Carrier gas Air Carrier gas flow 60 l / min Outside pressure atmospheric Diameter of the central electrode 3 mm Diameter of the central channel at the zone of ignition 4 mm Diameter of section S1 8 mm Diameter of section S2 6 mm Diameter of section S3 4 mm Diameter of section S4 2 mm Length of each section 35 mm
- This example uses the device of the invention in its configuration represented on the Figure 1 .
- Energy source direct current Electrical voltage applied between the electrode and the housing 2 kV Carrier gas N2 / H2 Carrier gas flow 20 l / min Outside pressure atmospheric Diameter of the central electrode 3 mm Diameter of the central channel at the zone of ignition 4 mm Diameter of section S1 8 mm Diameter of section S2 6 mm Diameter of section S3 4 mm Diameter of section S4 2 mm Length of each section 35 mm
- This example uses the device of the invention in its configuration represented on the Figure 2 .
- This example uses the device of the invention in its configuration represented on the Figure 3 .
- This example uses the device of the invention in its configuration represented on the Figure 4 .
Abstract
Description
La présente invention concerne un dispositif de génération d'un flux de plasma possédant une température basse et une puissance relativement importante.The present invention relates to a device for generating a plasma stream having a low temperature and a relatively high power.
Dans le domaine du traitement des surfaces, il est connu d'utiliser un flux de plasma de manière, notamment, à souder des surfaces ou à découper des surfaces. De telles applications d'un flux de plasma ont notamment été décrites dans le brevet
La présente invention vise donc à proposer un dispositif permettant de générer un flux de plasma dont la température est basse tout en ayant une puissance relativement importante.The present invention therefore aims at providing a device enabling generate a plasma stream whose temperature is low while having a relatively high power.
A cet effet, conformément à l'invention, il est proposé un dispositif générateur d'un flux de plasma comprenant un boîtier électriquement conducteur de forme tubulaire formant un canal central traversé par un gaz tourbillonnant, une électrode centrale disposée coaxialement dans ledit canal et une source d'énergie électrique destinée à appliquer une tension électrique V entre l'électrode et le boîtier, caractérisé en ce que le diamètre moyen du canal formé par le boîtier diminue progressivement depuis une zone située sensiblement au niveau de l'extrémité libre de l'électrode jusqu'à une zone d'extrémité dudit boîtier, ladite zone d'extrémité étant configurée de telle sorte que la tension électrique minimale Vcmin(0) à appliquer pour développer un arc électrique entre ladite électrode et ladite zone d'extrémité soit strictement supérieure à ladite tension V.For this purpose, according to the invention, there is provided a device for generating a plasma flow comprising an electrically conductive box of tubular form forming a central channel through which a swirling gas passes, a central electrode disposed coaxially in said channel and a electric power source for applying an electrical voltage V between the electrode and the housing, characterized in that the average diameter of the channel formed by the housing decreases progressively from an area substantially at the free end of the housing electrode to an end zone of said housing, said end zone being configured such that the minimum electrical voltage Vcmin (0) to be applied to develop an electric arc between said electrode and said end zone is strictly greater at said voltage V.
D'autres configurations possibles du dispositif de la présente invention sont également définies dans les revendications 2 à 14.Other possible configurations of the device of the present invention are also defined in
Ainsi configuré, le dispositif selon l'invention permet de limiter le développement d'un arc électrique à l'intérieur d'un boîtier conducteur à une zone d'extrémité positionnée juste avant l'ouverture du boîtier destinée à délivrer le flux de plasma sur la pièce à traiter. En effet, la zone d'extrémité est configurée de telle sorte à développer un arc électrique avec l'électrode centrale uniquement à partir d'une certaine tension minimale. De ce fait, en appliquant une tension inférieure à ladite tension minimale, l'arc électrique se développe à l'intérieur du canal central du boîtier jusqu'à approcher, voire atteindre, ladite zone d'extrémité, puis se rétracte brusquement en direction de l'électrode centrale. Par la suite, il reprend son développement à l'intérieur du canal en direction de ladite zone d'extrémité jusqu'à ce qu'il se rétracte à nouveau. Cette succession de développement et de rétractation de l'arc électrique génère au final un flux de plasma relativement puissant mais dont la température est suffisamment basse pour permettre son utilisation dans de nombreuses applications de traitement de surface.Thus configured, the device according to the invention makes it possible to limit the development of an electric arc inside a conductive casing to an end zone positioned just before the opening of the casing intended to deliver the flow of plasma over the piece to be treated. Indeed, the end zone is configured so as to develop an electric arc with the central electrode only from a certain minimum voltage. Therefore, by applying a voltage lower than said minimum voltage, the electric arc develops inside the central channel of the housing to approach or even reach said end zone, then retracts abruptly in the direction of the central electrode. Subsequently, it resumes its development inside the channel towards said end zone until it retracts again. This succession of development and retraction of the electric arc ultimately generates a relatively powerful plasma flow but whose temperature is low enough to allow its use in many surface treatment applications.
D'autres avantages et caractéristiques de la présente invention seront mieux compris à la lecture d'un mode particulier de réalisation de l'invention et en référence aux dessins dans lesquels:
- la
Figure 1 représente une vue schématique, latérale et en coupe d'un dispositif générateur d'un flux de plasma selon l'invention; - la
Figure 2a représente une vue schématique, latérale et en coupe d'une première variante d'une zone d'extrémité utilisable dans le dispositif représenté à laFigure 1 ; - la
Figure 2b représente une vue de face de la zone d'extrémité représentée à laFigure 2a ; - la
Figure 3a représente une vue schématique, latérale et en coupe d'une deuxième variante d'une zone d'extrémité utilisable dans le dispositif représenté à laFigure 1 ; - la
Figure 3b représente une vue de dessus de la zone d'extrémité représentée à laFigure 3a ; - la
Figure 3c représente une vue de dessus de la zone d'extrémité représentée à laFigure 3a , dans sa position d'utilisation; - la
Figure 4 représente une vue schématique, latérale et en coupe d'une troisième variante d'une zone d'extrémité utilisable dans le dispositif représenté à laFigure 1 ;
- the
Figure 1 represents a schematic side view in section of a device generating a plasma flow according to the invention; - the
Figure 2a represents a schematic, lateral and sectional view of a first variant of an end zone that can be used in the device represented in FIG.Figure 1 ; - the
Figure 2b represents a front view of the end zone shown in FIG.Figure 2a ; - the
Figure 3a represents a schematic, lateral and sectional view of a second variant of an end zone that can be used in the device represented in FIG.Figure 1 ; - the
Figure 3b represents a view from above of the end zone shown in FIG.Figure 3a ; - the
Figure 3c represents a view from above of the end zone shown in FIG.Figure 3a in its position of use; - the
Figure 4 represents a schematic, lateral and sectional view of a third variant of an end zone that can be used in the device represented in FIG.Figure 1 ;
Le dispositif 10, représenté sur la
La structure de base du dispositif 10 telle que décrite ci-dessus ne permet toutefois pas la génération d'un flux de plasma de faible température. En effet, dans cette structure de base, l'arc électrique 12 se stabilise rapidement. Le flux de plasma est donc généré sans interruption tant qu'une tension V est maintenue entre l'électrode 5 et le boîtier 1. Ce mode de fonctionnement induit la formation d'un flux de plasma puissant et particulièrement chaud. En outre, dans cette configuration, le risque est grand que l'arc électrique 12 se forme directement entre l'électrode 5 et l'objet à traiter si ce dernier est métallique. Pour remédier à cela, la Demanderesse a eu l'idée de limiter le développement de l'arc électrique 12, notamment en provoquant sa rétractation dès qu'il atteint une zone limite à l'intérieur du boîtier 1. Il s'avère que, pour maintenir une puissance suffisante au flux de plasma, il est avantageux de faire coïncider cette zone limite avec la zone d'extrémité 13 mentionnée précédemment.The basic structure of the device 10 as described above, however, does not allow the generation of a low temperature plasma stream. Indeed, in this basic structure, the
A ce stade, deux solutions peuvent être envisagées pour provoquer une rétractation de l'arc électrique 12.At this stage, two solutions can be envisaged to cause a retraction of the
Une première solution consiste à déterminer d'abord la tension réelle Vcmax à partir de laquelle un arc électrique est susceptible de se former entre l'électrode 5 et la zone d'extrémité 13 du boîtier 1. En contrôlant la tension réelle Vr au moyen du dispositif 8, il est possible de déterminer à quel moment Vr atteint la valeur Vcmax. Le dispositif 8 est alors capable d'envoyer un signal d'interruption à la source de tension 7 de façon à produire une micro-coupure électrique qui entraîne une rétractation de l'arc 12 jusqu'à la zone d'ignition 9. Par la suite, le rétablissement et le maintien de la tension V produit à nouveau l'expansion de l'arc 12 jusqu'à la zone d'extrémité 13 et, par conséquent, à nouveau sa rétraction. En procédant de cette façon, on génère un flux de plasma non équilibré qui se caractérise par une température relativement basse, notamment comprise entre 30°C et 300°C.A first solution is to first determine the actual voltage Vcmax from which an electric arc is likely to form between the
Une deuxième solution consiste à configurer le dispositif générateur du flux de plasma de telle sorte qu'une rétraction automatique de l'arc électrique 12 se produise au moment où il atteint ou approche la zone d'extrémité 13. Ce résultat peut notamment être obtenu en utilisant la structure particulière du boîtier 1 représenté sur la
En référence aux
Dans cette variante, la zone d'extrémité 13 définit un canal d'extrémité orienté selon l'axe longitudinal du boîtier 1, ledit canal d'extrémité débouchant sur une extrémité ouverte 14 de forme conique par laquelle sort le flux de plasma. De cette façon, on constate que les micro-arcs 11 sortent du canal d'extrémité 13 en suivant la surface conique de ladite extrémité 14. Cette répartition uniforme des micro-arcs 11 à la surface du cône génère au final un flux de plasma plus large et moins intense qui permet de diminuer encore sa température et permet d'utiliser le dispositif 10 sur un éventail plus large de surfaces. Dans une configuration préférentielle de l'invention, il sera avantageux de configurer l'extrémité ouverte 14 de telle sorte que sa forme conique définisse partiellement une hyperboloïde de révolution et que le rapport entre le diamètre extérieur du cône et le diamètre de la paroi interne du boîtier 1 au niveau du canal d'extrémité 14 soit compris entre 2 et 20.In this variant, the
En référence aux
Dans cette variante, la zone d'extrémité 13 définit un canal d'extrémité orienté selon l'axe longitudinal du boîtier 1, ledit canal d'extrémité débouchant sur un canal 15 ouvert à ses deux extrémités 16 et formant un angle α avec l'axe longitudinal du boîtier 1, l'angle α étant inférieur ou égal à 90°. Dans la configuration représentée, cet angle α est sensiblement égal à 90°. De cette façon, le flux de plasma F sort du boîtier 1 par deux ouvertures 16 formées sur ses parois latérales et selon une direction transversale à l'axe longitudinal du boîtier 1. Cette configuration permet d'appliquer plus facilement le flux de plasma F à l'intérieur de tubes ou, plus généralement, à l'intérieur d'objets creux. Par ailleurs, comme représenté sur les
En référence à la
Dans cette variante, la zone d'extrémité 13 définit un canal d'extrémité orienté selon l'axe longitudinal du boîtier 1, ledit canal d'extrémité possédant une pluralité d'ouvertures 18 débouchant sur une pluralité de canaux transversaux 19 orientés de manière sensiblement perpendiculaire à l'axe longitudinal du boîtier 1 et dont l'une des extrémités 20 est ouverte. Le flux de plasma F sort donc par chacune desdites extrémités ouvertes 20. Cette répartition en "peigne" du flux de plasma F permet donc de traiter plus facilement des surfaces larges. Par ailleurs, du fait que le flux de plasma sortant des ouvertures 20 possède une intensité variable selon la position des ouvertures 20 dans le canal d'extrémité 13, il peut être avantageux de pratiquer une ouverture supplémentaire 21 à l'extrémité du canal d'extrémité 13 de façon à laisser sortir partiellement ledit flux de plasma à travers ladite ouverture 21 et ainsi uniformiser l'intensité des flux de plasma sortant des ouvertures 20.In this variant, the
À titre indicatif, divers exemples de réalisation du dispositif de l'invention sont donnés ci-dessous.As an indication, various embodiments of the device of the invention are given below.
Cet exemple utilise le dispositif de l'invention dans sa configuration représentée sur la
Il se produit une succession de développement-rétractation d'un arc électrique entre l'électrode centrale et la section S4 à la fréquence de 2 kHz.There is a succession of development-retraction of an electric arc between the central electrode and the section S4 at the frequency of 2 kHz.
Cet exemple utilise le dispositif de l'invention dans sa configuration représentée sur la
Il se produit une succession de développement-rétractation d'un arc électrique entre l'électrode centrale et la section S4 à la fréquence de 1,5 kHz.There is a succession of development-retraction of an electric arc between the central electrode and the section S4 at the frequency of 1.5 kHz.
Cet exemple utilise le dispositif de l'invention dans sa configuration représentée sur la
Il se produit une succession de développement-rétractation d'un arc électrique entre l'électrode centrale et l'extrémité du cône à la fréquence de 4 kHz.There is a succession of development-retraction of an electric arc between the central electrode and the end of the cone at the frequency of 4 kHz.
Cet exemple utilise le dispositif de l'invention dans sa configuration représentée sur la
Il se produit une succession de développement-rétractation d'un arc électrique entre l'électrode centrale et la section S4 à la fréquence de 3 kHz.There is a succession of development-retraction of an electric arc between the central electrode and the section S4 at the frequency of 3 kHz.
Cet exemple utilise le dispositif de l'invention dans sa configuration représentée sur la
Il se produit une succession de développement-rétractation d'un arc électrique entre l'électrode centrale et le canal d'extrémité à la fréquence de 1 kHz. Cette configuration a permis d'obtenir des jets de plasma de densité identique et orientés selon une direction perpendiculaire à l'axe du canal central ce qui permet de traiter des surfaces larges.There is a succession of development-retraction of an electric arc between the central electrode and the end channel at the frequency of 1 kHz. This This configuration made it possible to obtain plasma jets having the same density and oriented in a direction perpendicular to the axis of the central channel, which makes it possible to treat large areas.
Claims (14)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CH01932/08A CH700049A2 (en) | 2008-12-09 | 2008-12-09 | Method and device for generating a plasma stream. |
EP09775312.3A EP2377373B1 (en) | 2008-12-09 | 2009-12-08 | Method for generating a plasma flow |
Related Parent Applications (1)
Application Number | Title | Priority Date | Filing Date |
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EP09775312.3 Division | 2009-12-08 |
Publications (1)
Publication Number | Publication Date |
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EP2613614A1 true EP2613614A1 (en) | 2013-07-10 |
Family
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Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
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EP09775312.3A Not-in-force EP2377373B1 (en) | 2008-12-09 | 2009-12-08 | Method for generating a plasma flow |
EP13162477.7A Withdrawn EP2613614A1 (en) | 2008-12-09 | 2009-12-08 | Device for generating a plasma stream |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
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EP09775312.3A Not-in-force EP2377373B1 (en) | 2008-12-09 | 2009-12-08 | Method for generating a plasma flow |
Country Status (6)
Country | Link |
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US (1) | US8847101B2 (en) |
EP (2) | EP2377373B1 (en) |
CH (1) | CH700049A2 (en) |
DK (1) | DK2377373T3 (en) |
ES (1) | ES2421387T3 (en) |
WO (1) | WO2010067306A2 (en) |
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PL2359061T3 (en) * | 2008-12-12 | 2019-02-28 | Sabaf S.P.A. | Gas burner for domestic cookers |
FR2962004B1 (en) * | 2010-06-24 | 2013-05-24 | Nci Swissnanocoat | DEVICE FOR GENERATING A PLASMA JET |
CN110087381A (en) * | 2011-03-25 | 2019-08-02 | 伊利诺斯工具制品有限公司 | Plasma torch system with improved plasma nozzle |
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EP0342388A2 (en) * | 1988-05-13 | 1989-11-23 | James A. Browning | High-velocity controlled-temperature plasma spray method and apparatus |
WO1996004098A1 (en) * | 1994-08-04 | 1996-02-15 | Sulzer Metco Ag | High velocity, high pressure plasma gun |
EP0994637A2 (en) * | 1998-10-16 | 2000-04-19 | Förnsel, Peter | Device for plasma treatment of bar or wire shaped material |
US20030047540A1 (en) * | 2001-09-07 | 2003-03-13 | Tepla Ag | Arrangement for generating an active gas jet |
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Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5233154A (en) * | 1989-06-20 | 1993-08-03 | Kabushiki Kaisha Komatsu Seisakusho | Plasma torch |
EP0729805B1 (en) * | 1992-11-27 | 1999-09-29 | Kabushiki Kaisha Komatsu Seisakusho | Plasma torch |
US5893985A (en) * | 1997-03-14 | 1999-04-13 | The Lincoln Electric Company | Plasma arc torch |
DE29805999U1 (en) * | 1998-04-03 | 1998-06-25 | Agrodyn Hochspannungstechnik G | Device for the plasma treatment of surfaces |
US6062492A (en) * | 1998-05-15 | 2000-05-16 | Sealant Equipment & Engineering, Inc. | Viscous material dispense system |
-
2008
- 2008-12-09 CH CH01932/08A patent/CH700049A2/en not_active Application Discontinuation
-
2009
- 2009-12-08 EP EP09775312.3A patent/EP2377373B1/en not_active Not-in-force
- 2009-12-08 ES ES09775312T patent/ES2421387T3/en active Active
- 2009-12-08 DK DK09775312.3T patent/DK2377373T3/en active
- 2009-12-08 US US12/998,872 patent/US8847101B2/en not_active Expired - Fee Related
- 2009-12-08 WO PCT/IB2009/055571 patent/WO2010067306A2/en active Application Filing
- 2009-12-08 EP EP13162477.7A patent/EP2613614A1/en not_active Withdrawn
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3515839A (en) | 1967-04-07 | 1970-06-02 | Hitachi Ltd | Plasma torch |
US3914573A (en) * | 1971-05-17 | 1975-10-21 | Geotel Inc | Coating heat softened particles by projection in a plasma stream of Mach 1 to Mach 3 velocity |
EP0342388A2 (en) * | 1988-05-13 | 1989-11-23 | James A. Browning | High-velocity controlled-temperature plasma spray method and apparatus |
WO1996004098A1 (en) * | 1994-08-04 | 1996-02-15 | Sulzer Metco Ag | High velocity, high pressure plasma gun |
EP0994637A2 (en) * | 1998-10-16 | 2000-04-19 | Förnsel, Peter | Device for plasma treatment of bar or wire shaped material |
US20030047540A1 (en) * | 2001-09-07 | 2003-03-13 | Tepla Ag | Arrangement for generating an active gas jet |
Non-Patent Citations (1)
Title |
---|
"Surface Treatment of Plastics by Plasmajet", JOURNAL OF ADHESION SOCIETY OF JAPAN, vol. 6, no. 4, 2 August 1968 (1968-08-02) |
Also Published As
Publication number | Publication date |
---|---|
US8847101B2 (en) | 2014-09-30 |
US20110240460A1 (en) | 2011-10-06 |
CH700049A2 (en) | 2010-06-15 |
WO2010067306A3 (en) | 2010-08-12 |
ES2421387T3 (en) | 2013-09-02 |
EP2377373B1 (en) | 2013-04-17 |
WO2010067306A2 (en) | 2010-06-17 |
EP2377373A2 (en) | 2011-10-19 |
DK2377373T3 (en) | 2013-07-22 |
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