The invention relates to an oscillating-piston drive for a vacuum pump with a piston, which presents two piston sections and an intermediate zone provided with a drive magnet, cylinder sections associated to said piston sections, an annular recess arranged between the cylinder sections at a central yoke, said recess forming the space for movement of said drive magnet and an electromagnetic drive surrounding the piston, which comprises yoke components and coils situated to the sides of said central yoke. Moreover, the present invention relates to an operating method for the drive.
Generally it is the aim of the here affected developers and designers to improve the delivery rate or effect (pumping capacity, compression) of a vacuum pump while simultaneously maintaining or even reducing, if possible, the construction volume and/or preferably even reducing energy consumption. This aim is equivalent in that in the course of the further development, respectively design of a pump of the affected type, measures which become necessary must not be associated with impairments affecting the delivery rate.
It is the task of the present invention to propose an oscillating piston drive for a vacuum pump in which delivery rate impairments are reduced.
This task is solved through the present invention through the characterising features of the patent claims.
An oscillating piston drive of the aforementioned kind is known from WO 00/63 556, drawing
By means of a first solution for the posed task, it is proposed that a can delimits peripherally the outer recess. A pipe section peripherally delimiting the space for movement of the drive magnet reduces the number of slots opening out into the space for movement so that the risk of unwanted pressure increases in this volume is substantially removed. The wall thickness of the pipe may be very small, below 1 mm, for example, so that impairments in the efficiency of the electromagnetic drive are negligible.
Expedient materials for the can are those which offer good sliding properties, like plastic, aluminium, stainless steel1) or alike (not—or only weakly ferromagnetic)2).
1) Translator's note: The German text states “Edelstahlt” here whereas “Edelstahl” would be appropriate. Therefore the latter has been assumed for the translation.
2) Translator's note: In the German text the right bracket is missing. It has been added to the translation.
Alternatively the can may consist of a more strongly ferromagnetic material, and its wall thickness selected at least in the area of the sections outside the central yoke such that the drive magnet magnetises the respective section to the saturation point when it is located in the zones outside of the central yoke. This embodiment of the can has the effect that it at least partly becomes part of the drive. The in each instance saturated section is practically no longer existent for the magnetic field of the related coil. This has an effect equivalent to an enlargement of the air gap for this coil and results in a reduction in the inductance of specifically this coil. The current in a coil is built up when the drive magnet is located in the area of this coil, i.e. the corresponding can section is saturated. Lower inductance means faster current build-up at a given voltage. With the magnetic field of this current, now the drive magnet of this coil is repelled towards the axially opposing coil. The saturation effect of the drive magnet on the can disappears. But since the current now has the required level, the increase in inductance is not disturbing.
This operating principle requires that the magnetic field of the drive magnet be stronger compared to that of the coil. If this were not the case, then the field of the coil would practically “overwrite” the field of the drive magnet in the can (the directions of the fields oppose each other) thereby cancelling the saturation immediately. In the instance of this drive, the necessary forces may, however, only be implemented by sufficiently strong rare earth magnets, for example. In the instance of these magnets this requirement is always fulfilled.
From the above descriptions it is apparent that it is expedient to control the current through the coils such that a current is allowed to flow only through one coil at a time. In this manner it is achieved that the current in one coil is built up precisely when the drive magnet is located in the area of this coil.
Controlling the drive by means of semiconductor switches allows the avoidance of further losses. To explain this improvement, the existence of a linear drive in accordance with drawing
In a second solution for the task of the present invention it is proposed that only one current polarity be assigned to each of the coils, i.e. the positive current polarity is assigned to one coil and the negative current polarity to the other. For example, the two polarities of the 50 Hertz mains AC can be “distributed” to both coils.
This may be implemented with a simple thyristor regulator. The current amplitude of each half-wave may be adjusted by means of a simple, cost-effective phase angle regulator, as is known from electric drilling machines, for example.
The input signal for the phase angle regulator may for example be
The frequency of the piston's stoke will in all cases result from the frequency of the supplied alternating current.
The advantages of these measures are on the one hand that losses in the coils are reduced, since the current is allowed to flow only through one coil at a time. Also the implementation of the control electronics is more simple, since it is no longer required for the currents to flow simultaneously through both coils.
Further advantages and details of the present invention shall be explained with reference to the examples of embodiments depicted in the drawing FIGS. 1 to 3.
Depicted is in
The drawing figures each depict a piston vacuum pump 1 with a piston 2. This exhibits piston sections 3 and 4, to the unoccupied face sides of which each a cylindrical pump chamber 5, respectively 6 is assigned. The piston 2 and the pump chambers 5, 6 are located in a housing 7 with cylinder sections 8, 9 for the piston sections 3, 4. The materials for the sliding cylinder surfaces and the corresponding piston surfaces are selected in a basically known manner such that the pump may be operated dry, i.e. without lubricant.
A linear drive is assigned to the piston 2. Said linear drive comprises on the side of the piston a permanent magnet ring 11, encompassing the piston 2 at its central zone. The permanent magnet ring 11 moves in the annular volume (recess 12) encompassing the piston 2. On the stator side, further permanent magnet rings 13, 14 are assigned to the permanent magnet 12 on the side of the piston, said further permanent rings axially delimiting the annular recess 12. At the level of these permanent magnetic rings, also cylinder sections 8, 9 terminate.
Moreover, the coils 15 and 16 are components of the linear drive on the stator side. These are partly encompassed by yoke components 17, 18 and jointly with these yoke components said coils encompass the cylinder sections 8, respectively 9. Located between the coils 15, 16 and the yoke components 17, 18 is an annular center yoke 19, the inner surfaces of which face the annular chamber 12. Currents are made to flow through coils 15, 16 such that the magnetic field produced by the coils and guided by the yoke components 17 to 19 interact with the magnetic fields of the permanent magnet rings 11, 13 and 14 in the desired manner. The piston 2 shall oscillate about its centre position such that during this movement the face sides of the piston may fulfil their pumping function.
For the purpose of fulfilling the desired pumping effect, the compression chambers 5, 6 are each equipped with an inlet valve and an outlet valve (only depicted in drawing
In all, two compression stages are present. They may be operated in series or in parallel. Details on this are not presented.
In all drawing figures the can is designated as 34. It encompasses the annular chamber, respectively the recess 12, and extends into the area of the stator permanent magnet rings 13, 14.
Drawing
Drawing
Expediently the coils 15, 16 are switched on in the respective supply circuit in such a manner that they effect repelling forces on the drive magnet 11. Thus the piston will oscillate about its central position at the frequency of the supplied alternating current.
The permanent magnets 13, 14 are expediently magnetised such that they will effect on the drive magnet a repelling action. This solution offers the advantage that mechanical springs which move the piston back to its central position can be omitted.
Number | Date | Country | Kind |
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101 49 506.4 | Oct 2001 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP02/10921 | 9/28/2002 | WO |