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Surface processing by arc discharge in vacuum. RU patent 2509824. |
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IPC classes for russian patent Surface processing by arc discharge in vacuum. RU patent 2509824. (RU 2509824):
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FIELD: metallurgy. SUBSTANCE: arc discharge cathode spots are initiated at processed surface, arc discharge being initiated between anode and cathode in the mode of voltage-current characteristic of increasing section, said cathode being a processed surface. Region of cathode spot location on processed surface is localised and processed surface is shifted by anode displacement. Anode with current-collecting surface area smaller than that of cathode is used and placed at the distance from cathode that ensures a positive anode voltage drop. EFFECT: stabilised cathode spots on processed surface, fast surface cleaning and higher surface quality. 2 dwg
The claimed invention relates to the technique of surface treatment products arc discharge in vacuum to remove surface dirt. Currently, cleaning products are widely applied to various mechanical, chemical and electrochemical methods. Depending on the nature, type and degree of contamination primarily used aqueous detergents and solvents, an organic liquids of different polarity (benzene, kerosene, acetone, ethylene dichloride, and others). Used for this purpose production line treatment, require large areas. Released during the etching of evaporation is not only harmful for staff, but also destructive influence on production equipment at shop design. In addition, the use of acids and alkalis requires their disposal, subject to measures preventing the environment pollution. To clean the surface of the material from residues of lubricants, descaling, oxide films and other types of contaminants are widely used arc discharge in a vacuum. In comparison with other methods, this method is attractive because of its absolute environmental safety and because of the number of benefits arising from the effect of the discharge on the surface. The electric arc is established form of electric current passing through the discharge gap and bordering electrodes, low cathode voltage drop (about potential excitation or ionization of atoms plasma environment) and large bit currents. Arc categories differ in the character of physical processes at the cathode, the state plasma positive column, and also by the nature and pressure of plasma-forming medium through which the current flows. For all types of arc discharge regardless of the pressure plasma environment width of the region of the cathode voltage drop d to significantly shorter than the mean free path of electrons λe , because what is the latest cross it in the collisionless regime. In [Lisenkov A.A. Cathode spot of vacuum arc discharge // Vacuum equipment and technology, 2004. T. №4. S-226] it is shown that in case of vacuum-arc discharge, at the initial moment of time on crude cathode surface occurs uncontrollable, chaotic and moving very quickly covering the entire surface of the discharge. The presence of surface impurities and defects even at low concentrations has a significant influence on thermal emission properties of metals and leads to a noticeable variation output (more than 0.1 eV). These conditions significantly facilitate the maintenance of an emerging category that can exist at a lower value of the discharge current than the discharge cathode material. Discharge current determines the number of spots simultaneously existing on the working surface of the cathode. So thin-film coatings pollution, current, mud at each cathode spot, can be supported by a current of a few amps, what with the increase of the discharge current is increasing simultaneously existing stains. Under the high density of energy released in the cathode spots, is local heating of the surface, explosive evaporation layer of dirt and formation generated from treated surfaces plasma flows. The number of known ways of processing of a surface of products arc discharge in a vacuum: - the impact of the arc discharge on the surface in vacuum at a pressure of 10 -5 ...10 -3 mm Hg [speaker of the Russian Federation №476041. B08B 1/00. Esteros - and other The way to remove the oxide film and dirt from the details lei; application №1695276, 30.08.1971. Publ. 05.07.1975, bul. №25]; - the impact of the arc discharge to the surface being treated in a protective gas environment [speaker of the Russian Federation №171056. H05B. Finland L.A., leschev E.N. The method of purification of arc wire arc welding; application №818848/25-27, 19.11.1963. Publ. 11.05.1965]. When burning arc discharge observable physical processes are determined by the behavior of cathode spots, which are fundamentally unstable plasma formations and are characterized by some average life time. The main task for the removal of surface dirt is the creation of devices managed by the nature of the movement of cathode spots on the working surface. In [RF Patent 2180472. H05H 1/50, C23C 14/35. Lisenkov A.A. and other Vacuum-arc plasma source; application №20001103758/06, 07.02.2000. Publ. 10.03.2002] it is shown that at operation of control devices on the cathode surface arise velocity of cathode spots, which, despite the presence of an external magnetic field, carry out the chaotic movement across the surface of the cathode with the purpose of cleaning, including its outside part where and created the ideal conditions for maintaining discharge between the cathode and the anode. In [ASF №1695704. C23C 14/02. Esteros - and other Method of surface treatment products arc discharge in a vacuum; application №4339958, 21.12.1987. Publ. 23.12.1992] for removal from a surface of details oxide films and pollution, hardening or leave the near-surface layer machined parts, remove Burr, moving cathode spots on the surface, is performed by moving the screen with a hole, located between the cathode and the anode. The use of the screen with aperture, requires a significant increase in power is invested in the discharge. The intensity of the plasma flows from the diaphragm exceeds the intensity of the cathode and anode jets, which shifts the region of their interaction to the electrodes and contributes to the formation of diffuse binding arc to the electrodes. The screen in the process of work intensively heated, which requires cooling, which is hard to arrange in a vacuum. Move the screen above the surface very difficult to operate and requires creation of complex systems of electrical insulation. The method of cathodic treatment of details sustainable arc discharge [A.S. the Russian Federation №719710. B08B 3/10, H05B 7/00. Esteros - and other application 2569061, 01.12.1977. Publ. 05.03.1980] - discharge is burning between the anode and the cathode (the workpiece) mode of declining area of volt-ampere characteristics. To improve the speed and quality of treatment in the process of surface treatment changes the potential along the treated surface. Thereby provides directional movement cathode spot. The disadvantage of this method is the low quality of surface cleaning products and low productivity due to the possibility of existence of two types of sustainable arc discharge in vacuum, depending on the nature of physical processes in the field of cathode and anode spots. The closest to the claimed method on a set of attributes is the method of surface treatment products arc discharge in vacuum, is presented in [RF Patent №2144096. C23C 14/02, C23F 4/04. Of Antibes B.F. and. other The method of surface treatment products arc discharge in a vacuum; application №981100036/02, 18.05.1998. Publ. 10.01.2000]. Localization of cathode spots of the arc discharge on the treated surface in vacuum is achieved by imposing a constant magnetic field. Arc discharge excite mode growing area of volt-ampere characteristics, which distinguish between the cathode and anode region and nestled in between the positive pole. To control the movement of cathode spots on the electric arc is applied external magnetic field, while, due to changes in the magnitude and direction of the magnetic induction vector. Moving cathode spots on a processed surface requires the creation of complex mechanical systems and control systems for moving magnetic systems. Besides these conditions significantly limit the field of practical application of the method for machining of complex components. Task the claimed invention is a method of surface treatment products arc discharge in vacuum with reliable fixation and managed nature move cathode spots on the surface that would be easy to use and versatile in application for surface treatment any geometric forms. The solution of this problem will allow to achieve the following technical results: - to simplify the stabilization of cathode spots on the treated surface; - reducing the time of technological process of purification; - to improve the quality of the surface. Specified the technical result is achieved due to the fact that the method of surface treatment products arc discharge in vacuum, including initiation on the treated surface of the cathode spots of the arc discharge, which excite mode growing area of volt-ampere characteristics between the anode and cathode, which is treated surface, for the implementation of the localization region of existence of cathode spots on the treated surface and its offset by moving the anode, while using the anode area tokopriemnye surface, the smaller area of the cathode, and install it on the distance from the cathode providing positive anode voltage drop. The implementation of the stabilization of the discharge on the surface of treated using the selected combustion conditions of discharge is quite simple and does not require more complex design solutions, and to process the products of any shape, including sample plots available hard surfaces. Summary of the invention is illustrated by drawings. Fig 1. - Vacuum-arc device for surface treatment products cathode spots of the arc discharge in vacuum and distribution voltage between the electrodes. 2. - Photo of the processed surface. The device that implements the method of surface treatment products cathode spots of the arc discharge in vacuum, presented in (Fig 1, a). The expansion of the plasma flow in the area of the anode 2 is in the direction, first of all perpendicular to the surface of the cathode 1, which formed the cathode spot 3, the longer the distance from the cathode 1 to the anode 2, the greater the receiving surface shall to have the anode 2. To initiate the cathode spots of the arc discharge pulse is used scheme of control electrode 4, which with the specified frequency and amplitude pulses U under . Depending on the implemented design might as moving anode 2 regarding processed surface 1, and move the cathode 1 regarding the anode 2. The minimum distance between the electrodes (L CA ) is determined by the region of localization of the arc discharge and conditions effective electronic circuit current from the cathode to 1 on the anode 2 (in the process of work, provided move the electrodes relative to each other, the distance L CA remains unchanged). The distribution of the electric field in such a system is determined by the voltage at the electrodes, the specific conductivity of plasma and spatial distribution of the space charge in the near-electrode regions. The presence of non-compensated charge shall determine the existence of near-cathode (U ) and anode (U a ) potential drop (Figure 1, b). The General decline in arc voltage (L arcs ) is the sum of the voltage on the arc column (U V. ), cathode (U ) and an anode (U and - a potential difference between the edge the area undisturbed anode phenomena positive post and anode): U Doug =U +U a +U V. Under the condition of homogeneity of the arc column, U article is defined as the product of the electric field strength E on the length of the channel arc l U St =El. In the vacuum-arc plasma sources used for formation of coatings, the distance between the cathode and the anode (CA L ) reaches 0.5 m For effective as cleaning the surface of the cathode spots and stable combustion discharge, the distance between the electrodes does not exceed a few centimetres. Between the unperturbed plasma and anode 2, is formed near-electrode layer of the space charge (Figure 1, b) - anode voltage drop (U a )regulating the flow of charged particles on the anode: U a = - k T e e ln j e j a ,where k - Boltzmann constant; T e - e-temperature; 1/2 j e =0,25en(8kT e /πm e ) 1/2 - density chaotic current of electrons from the plasma; j a =I bit /S a is the density of the discharge current on the anode; S a reception surface of the anode; I time - discharge current. As you can see, the sign of the anode voltage drop (U a ) depends on the ratio of currents j e /j a, and can be both positive and negative. If the total current, resulting integrating current density of chaotically moving plasma electrons across the surface of the anode, was equal to the required current (j e =j (a ), then this is the ideal case U a =0. Negative drop is implemented, provided j e S a >I once (j e >j a ) and is provided at the discharge current I (for all the considered cases believe that I =const), and the developed surface of the electrode (S <<S a ), which adjoins dense, strongly ionized plasma. These conditions are implemented in a vacuum-arc plasma sources used for coating. In this case, the negative anode drop is small at (-1 -3...) Century With the reduction of the area of the anode (S & GE; S a ), if / once and the corresponding change of density currents j and e j a , this shell first disappears (while I, a =j e S a a U a =0), and then is replaced by electronic. The change of sign anode potential drop occurs when J e S a <I times : reception of the surface of the anode S a reduced ('s to >>S a ), and the current density j a is equal to or greater j e . Involved in the way the area of the electrode is selected from the following conditions: S a < 4 I R and C e n e 8 k T e / PI m e exp ( - e U a k T e )Thus, the anode potential drop (U a ), its sign and magnitude are to control that supports the concentration of charged particles before the anode at the level providing summing to it the discharge current. The sign and magnitude of anode voltage drop (U a ) depend on the shape and size of the receiving surface of the anode 2, the distance between the electrodes (L CA ), on the degree of vacuum in a vacuum chamber, the presence of gas, the discharge current (I ) and some other factors. In the discharge anode small square near the anode there is a strong electric field, dilatory from him ions. When the rate of formation of ions is the same as in the post, negative space charge cannot be compensated for and installed the positive anode drop of this magnitude, which accelerated during the electrons produce additional ionization, supplying the required amount of ions. In addition to electrons hitting the anode 2 with energy corresponding to the anode potential drop (U a ), condensed and release energy neutral atoms of metal, and also reported to the radiation energy cathode and plasma flow. All incoming energy must be balanced by the heat sink deep into the anode 2, reverse radiation in the category and evaporation anode or other materials, condensing metals. For calculation of the power, generated at the anode (P (a ), the expression where I once discharge current, reaching the anode; eφ - the work of an electron exit of the anode material; 2kT e /e is the average kinetic energy of the electrons produced in the anode region of plasma; U a - anode voltage drop. The cleaning mode on the contaminated areas of the working surface of the cathode exists independent, chaotic and fast-moving category. At the moment of time t=0 (Fig 1, a) for initiating the electrode 4 is served pulse voltage U under , contributing to the formation on the cathode surface 7 source primary electron - cathode spots 3, which is the basis of post arc discharge. Number of simultaneously existing cathode spots is determined by the discharge current I , the degree and type of soiling of the surface. After excitation - cathode spot 3, moving in an external electric E →and self-magnetic B →the fields are retained on the part of the surface cathode 7, where there is a minimum voltage of burning discharge, i.e. in the field with a minimum distance of anode-cathode L CA , and provide the most favorable conditions for the closure of the discharge current on the surface of the anode 2. Thus, the movement of cathode spots on 3 processed surface (S ) is determined by the place of arranging the anode 2 regarding cathode 7 and localization of cathode spots limited to geometric size of the receiving surface of the anode S a . Moving cathode spots 3 on the treated surface is chaotic and therefore the reduction of the receiving surface of the anode 2 limits the surface of the containment area is equivalent ~ S a . Narrowing the field of existence increases as the speed of rise of temperature on the treated area of the cathode 1, and the rate of removal of dirt from the surface. The time spent anode relative to the treated surface is determined by the density of the heat flux q emitted by cathode spots, and a level surface contamination at the site. In the result of the cathode spot 3 (temperature exceed boiling temperature, the material on where they exist) provide as evaporation of the surface layer (layer of dirt), and heat the surface up to the temperatures at which in the areas adjacent to its location, there is the chemical decomposition of dielectric films and flaking scale. When considering heat problems, the unknown quantities are temperature distribution in the cathode 1, depth change warmed layer and the law of the time variation of the phase transitions. When considering the effects of moving cathode spot 3 on the surface in the presence of the processes of melting, crystallization and sublimation solution of the heat problem is reduced to the problem with moving boundary (Stefan problem). At the moment of time t 1 warranty 0 (Figure 1, b), provided move anode 2 with speed V a relatively cathode 7, observed motion of the cathode spots 3 on a processed surface in the direction appropriate to the offset of the anode. The velocity of an anode (V a ) with respect to the cathode 1 determined from the conditions of existence of the discharge on the cathode: discharge current (I ), thermophysical properties of the surface layer of the processed surfaces and conditions of heat removal. Anode shape 2 in the implementation of treatment is determined by the size and geometry of the processed surface 1 and at any point of the path, the distance between the surface 1 and anode 2 remains constant. The voltage drop across the discharge gap in the process of surface treatment in the presence of contamination and the existence of discharge purified cathode material is different. So the end of the treatment process is determined by the output on a stationary state of the voltage drop across the discharge gap. The technology was tested on the unit for removal of the outer surface of the steel cylinder (diameter 20 cm, length 50 cm) from contamination. Procurement is permanently attached to the structure, providing her forward motion of the anode, made in the form of water-cooled copper ring (inner diameter 22...25 cm, length 1,5...2,5 cm) and covering the surface. Procurement connected to the negative (grounded) terminal of the power source. The anode is connected to the positive terminal of the power source. Treatment in a vacuum chamber is carried out at a pressure of 1...10 PA. The voltage drop across the discharge gap for untreated surface was 17...20 In, and treated for more than 20 Century The created system allows you to modify the reception area of the surface of the anode 2 and the speed of travel of electrodes relative to each other, as well as current arc discharge, which allowed to study the relationship between the temperature of the arc and the temperature of the treated surface. Technology of cleaning of metal surfaces used for cleaning of large-size products, as well as in the restoration of various containers and pipelines gaseous and liquid media. The special importance of this technology gets when working with hazardous substances, as in the plasma flow is to decompose into less dangerous components. Thus, the proposed technology of processing of the surfaces with the arc discharge in vacuum improves quality, productivity and efficiency of the process, and most importantly, it meets the ecological requirements of modern manufacture. The method of surface treatment products arc vacuum discharge, including initiation on the treated surface of the cathode spots of the arc discharge, which arouse in the mode of increasing land-voltage characteristics between the anode and cathode, which is processed surface, wherein exercise localization region of existence of cathode spots on the treated surface and its offset by moving the anode, while using the anode area tokopriemnye surface, the smaller area of the cathode, and set him at a distance from the cathode providing positive anode fall voltage.
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