1. Field of the Invention
The present invention relates to a method for producing bores, e.g., in fuel injectors.
2. Description of Related Art
Such a method is used in particular for producing bores having relatively small diameters (so-called micro-bores) such as those used, for example, in injectors in internal combustion engines. For process-related reasons, however, material is also always removed from places on the workpiece where this is not desired. This is caused by electric fields related to the electrode geometry. Material is preferably removed from places having a relatively high electrical field strength because the current density is highest there. High field strengths occur primarily on sharp edges or corners, causing them to become eroded and rounded during processing. A higher conductivity of the working medium causes this effect to be all the more pronounced. For this reason, cylindrical bores having high precision, i.e., having as little material removal as possible on the edges of the bore in particular, are able to be produced using the known method only if an insulated electrode is used. However, to date, suitable insulation means allowing high stability with low insulation layer thicknesses are not available. For that reason, the production of such bores having small diameters is associated with relatively high costs.
An object of the present invention is to produce bores having a small diameter at high precision, in particular in the edge area of the bore, in a highly economical manner without using insulated electrodes.
The present invention is based on the idea of selecting the potential difference or the applied voltage between the two electrodes at such a high level that a gas-vapor envelope is produced around the tool forming the cathode via the electrolyte. This produces a field-free space between the gas-vapor envelope and the workpiece surface preventing material from being removed electrochemically, in particular in the opening area of the bore.
In an advantageous refinement of the present invention, the working voltage and thus the potential difference is varied, in particular pulsed. This also makes it possible to produce relatively small bores using a small tool without it being subjected to severe heat or increased wear.
In addition, it is possible to influence the wear of the tool in pulsed operation by appropriately prolonging the machining intervals in which no potential difference is present between the workpiece and the tool.
In pulsed operation, it is furthermore particularly advantageous to adjust the curve of the relative movement between the workpiece and the tool to the curve of the potential difference. This increases the precision of the machining process.
Identical elements and elements having the same function are denoted using the same reference symbols.
A conventional method for producing a bore 1 in a workpiece 10 is represented in
In the case of the method according to the present invention represented in
The entire system made up of workpiece 20 and tool 22 is located in a known manner in a production device 25 (not represented in greater detail) and is surrounded by an electrolyte 26 or an electrolyte solution. For example, electrolyte 26 has a conductivity greater than 10 mS/cm. When a working voltage is applied between the anode and cathode, denoted in the following as voltage Ua, the electrolysis causes hydrogen to be deposited on the cathode surface, i.e., on the surface of tool 22. According to the present invention, it is provided to select the potential difference between workpiece 20 and tool 22, i.e., voltage Ua at voltage source 21, at such a (high) level that the tool surface is completely surrounded by a gas-vapor envelope 27 which is at times penetrated by a plasma channel. In the case of small bore diameters, this is typically achieved at voltages Ua greater than 50 V. Similar to a thunderstorm, the plasma repeatedly penetrates gas-vapor envelope 27 at a consistently different location. If breakdown voltages occur, these are on the one hand breakdown voltages through gas-vapor envelope 27 between tool 22 and bore 1 within bore 1. Removal of material thus occurs only within bore 1 in this case. In the other breakdown voltages between electrolyte 26 and tool 22 outside of bore 1, the current first flows through the plasma channel, then through electrolyte 26 (U(electrolyte) not zero) and could result in the removal of material outside of bore 1. Since, however, the plasma limits the current flow (saturation effect), the current density on the workpiece surface is not sufficient for achieving removal of material. In the desired manner, this results in the formation of a relatively sharp-edged bore edge 33. It is noted in addition that a penetration through gas-vapor envelope 27 may also result in igniting of the hydrogen, primarily in the case of a penetration between tool 22 and workpiece 20, since both oxygen and hydrogen are in gas-vapor envelope 27 at this location.
Voltage Ua is broken down into a voltage component U(electrolyte) across electrolyte 26 and a voltage component U(pl) across the plasma. As seen in
The level of voltage Ua determines whether or not a plasma is formed. It has been found that the plasma ignites only very irregularly in the present example at voltages Ua of less than 70 V, so that the protection of the workpiece surface against electrochemical erosion is only partially present. For that reason, erosion occurs primarily at bore edge 33, since that is where the highest field strengths occur.
If, however, voltage Ua is increased to 105 V (at a conductivity of electrolyte 26 of 20 ms/cm), relatively sharp-edged bore edges 33 corresponding to
It is noted in addition that in the case of small tool/electrode diameters of approximately 100 μm, it is recommended to pulse voltage Ua, since otherwise the temperature on tool 22 may become so high in the presence of a direct voltage that it melts. The duration of pulse length and pulse interval (as well as voltage Ua) is in this case a parameter for influencing the intensity of the plasma. Shortening the pulse interval reduces the heating of the plasma. In long pulse intervals, the plasma is extinguished at times and an electrochemical erosion occurs on bore edge 33 (as is also the case at relatively low voltage Ua), which may be advantageously exploited. During the pulse intervals, it may be advantageous to reduce or stop the otherwise continuous feed motion of tool 22. Moreover, the relative velocity between tool 22 and workpiece 20 should advantageously be adjusted to the curve of voltage Ua to increase the bore's precision.
Using the method according to the present invention described above, it is thus possible in particular to produce high-precision bores having relatively small diameters (in particular having diameters smaller than 1 mm or a diameter to depth ratio of 1:10, so-called micro-bores), in particular in the opening area of the bores, without an insulated cathode (tool 22) being necessary for this purpose. However, in the case of a throttle bore, it is also possible to use the described method to produce the bore first, and subsequently widen the throttle bore electrochemically to the desired dimension in the same fixture of same production device 25 using same electrolyte 26, or round bore edge 33 of a micro-bore in a targeted manner (already in the boring process or also afterwards using a relatively low voltage Ua at which the plasma does not immediately ignite).
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2009 000 237.5 | Jan 2009 | DE | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/EP2010/050353 | 1/13/2010 | WO | 00 | 9/30/2011 |