(1) Field of the Invention
The present invention relates to a method and an apparatus for simultaneously heating materials by means of laser radiation, with an arbitrary shape of the substantially flat heating contour.
(2) Prior Art
It is known to heat materials by means of laser beams for the purpose of material shaping, for example for welding, soldering, cutting, etc. It is also known to connect plastics to one another by means of laser beams, for example using the laser transmission method. For welding purposes, the laser transmission method by means of IR radiation makes use of the different absorption in the parts to be welded to one another. The upper part, facing the laser source, is transparent to the laser beam, whereas the lower part absorbs the laser beam, and so because of the heating of the lower part the two components fuse at the welding point and are pressed together under pressure. Relatively fine and high-precision welds, in particular of micromechanical components, can be undertaken by means of the laser beam. It is advantageous to undertake the welding over the entire welding line simultaneously so that, during an exposure operation, the entire, substantially flat welding contour is heated and the components are welded to one another. In this way, the air gap between the components can be bridged during welding, and unevennesses can be balanced out.
It is therefore the object of the present invention to propose a method and an apparatus in which materials can be heated simultaneously in an arbitrary contour shape of the heating line by means of laser beams, in particular in which plastic components can be welded.
This object is achieved according to the invention by means of a method for simultaneously heating materials having an arbitrary, substantially flat shape of a heating contour by means of a laser radiation, comprising the steps of coupling a laser beam by means of optical elements in a longitudinal direction into a wall of a tube that is transparent to IR radiation and is deformed at an exit side in accordance with the heating contour, and imaging an emerging laser beam onto a heating plane by means of a converging lens and by means of an apparatus for simultaneously heating materials having an arbitrary shape of a substantially flat heating contour by means of laser radiation, comprising an optical arrangement for shaping a laser beam and for focusing the laser beam onto a tubular optical waveguide that is transparent to IR radiation and is deformed at an exit end in accordance with the heating contour and an adjoining means for focusing the emerging laser beam onto a heating plane.
In accordance with the method, the laser beam is coupled by means of optical elements in the longitudinal direction at the end side into the wall of a tube which guides IR beams and is deformed at the exit side in accordance with the contour, and the emerging laser beam is subsequently imaged onto the heating plane by means of a converging lens. The thin-walled tube shapes the beam, the tube being regarded not only as an optical waveguide and beam transformer, but also as homogenization means for the light intensity. For this purpose, the two ends of said thin-walled tube are highly polished in order to ensure that the laser beams are coupled in and coupled out without any losses. The circle circumference of the light-guiding tube corresponds to the desired overall heating contour length, thereby realizing most closed heating contours. The tube preferably remains in its round shape on one side of the tube. This side serves as an interface for coupling in light. The other side of the tube is shaped in a component-specific manner in order to produce the desired contour. The reshaping of this side may be realized in various ways, one possibility being for example to heat a plastic tube with hot air, to slightly soften the plastic and then to shape it into the desired contour figure by means of auxiliary shaping tools. Another type of shaping is production by means of injection-molding tools. Generally, all materials which ensure the above-mentioned functions are suitable, for example plastic, glass or tools based on glass.
In order to enable light to be coupled in in a homogenized manner, the laser radiation may preferably be reshaped annularly. In this case, the circle circumference of the ring should precisely correspond to the circle circumference of the plastic tube.
The annularly shaped laser radiation is advantageously achieved by means of an axicon lens. The latter transfers the laser light into an annular shape and it is subsequently focused sharply onto the cross section of the light-guiding tube by means of a downstream converging lens. As a result, the laser energy can be coupled into the light-guiding tube without any losses.
The laser beam, which emerges for example from an optical fiber, may be collimated onto the axicon lens via a converging lens. When the laser light emerges from the other side of the light-guiding tube, it will radiate out at a greater angle of divergence. Since there is an irreducible distance between the exit of the plastic tube and the heating plane, the exit figure is advantageously precisely imaged onto the heating plane again by means of a converging lens. This results in the desired working distance between the end side of the tube and the component. The homogenization of the beam intensity is improved by the length of the tube. The latter itself may be chosen in a variable manner.
The invention results in a high flexibility in the production of such a light-guiding tube as an optical tool. The formation of annular laser beams and the variation of the ring circumference can be realized relatively simply, so that the outlay for the production of such a complete device is low and thus highly advantageous.
This technique makes it possible, inter alia, for plastic components to be welded simultaneously, the progressive technique in which an ever higher laser power can be emitted from a point being advantageous. In this case, the fiber laser offers a small focusable spot size within 6 to 50 μm. The optical power of this type of laser can be scaled arbitrarily from a few watts up to a few kilowatts. As a result, this invention can be used technically in a broad field of application.
The invention is shown and explained in principle below on the basis of an exemplary embodiment in the case of welding plastic components in conjunction with the accompanying drawings, in which:
Number | Date | Country | Kind |
---|---|---|---|
03018970 | Aug 2003 | EP | regional |
Number | Name | Date | Kind |
---|---|---|---|
3419321 | Barber et al. | Dec 1968 | A |
4097118 | Hammer | Jun 1978 | A |
4799755 | Jones | Jan 1989 | A |
4824194 | Karasawa | Apr 1989 | A |
4941093 | Marshall et al. | Jul 1990 | A |
4941734 | Williams et al. | Jul 1990 | A |
5200230 | Poullos et al. | Apr 1993 | A |
5251060 | Uenishi et al. | Oct 1993 | A |
5261904 | Baker et al. | Nov 1993 | A |
5607730 | Ranalli | Mar 1997 | A |
5677920 | Waarts et al. | Oct 1997 | A |
5778133 | Plesko | Jul 1998 | A |
6004487 | Wada et al. | Dec 1999 | A |
6760973 | Koide | Jul 2004 | B1 |
6858104 | Flanagan | Feb 2005 | B2 |
6860960 | Flanagan | Mar 2005 | B1 |
20030128957 | Kalantar | Jul 2003 | A1 |
20040105482 | Sugiyama et al. | Jun 2004 | A1 |
Number | Date | Country |
---|---|---|
003904662 | Aug 1990 | DE |
0282593 | Sep 1993 | EP |
362151289 | Jul 1987 | JP |
402299791 | Dec 1990 | JP |
403170616 | Jul 1991 | JP |
403185776 | Aug 1991 | JP |
404012745 | Jan 1992 | JP |
404034505 | Feb 1992 | JP |
405069172 | Mar 1993 | JP |
405208258 | Aug 1993 | JP |
406262384 | Sep 1994 | JP |
2002283086 | Oct 2002 | JP |
02003121705 | Apr 2003 | JP |
WO9104829 | Apr 1991 | WO |
Number | Date | Country | |
---|---|---|---|
20050077276 A1 | Apr 2005 | US |