An apparatus according to the invention can basically be mounted at a bridge or a frame above the horizontal transporting device of a float glass installation. Two apparatuses which may share a temperature sensor 5 and a thickness sensor 6, as the case may be, are required to cut off both edges of a float glass ribbon 13 simultaneously.
As is shown in
By fastening the apparatus in a prescribed manner to a bridge or a frame 11 above the transporting belt, the cutting unit 11 and therefore in particular the beam-shaping optics 2, the cooling nozzles 4 and the scribing device 10 are positioned in a defined manner vertically and laterally with respect to the transporting device arranged horizontally below them. The scribing device 10, the beam-shaping optics 2 and the cooling nozzles 4 are arranged one behind the other at selected distances relative to one another in the transporting direction of the transporting device which is the same as the drawing direction of the float glass ribbon 13. Their vertical distance is regulated by the change in thickness so that they always maintain a constant distance from the float glass ribbon 13 moving on the transporting device regardless of the thickness of the float glass ribbon.
The cooling nozzles 4, three of which are provided in the embodiment example, can be opened individually or simultaneously so that the coolant can act locally over a shorter or longer period of time and the cooling penetrates to a varying depth from the surface into the material. The depth of the crack can also be influenced in this way, which is benefited by the fact that the material core is still warm.
The crack detector 7 is provided in order to ensure that a crack is always actually generated for the permanently and continuously running process. A radiation sensor which emits a measurement beam that is reflected back into the sensor at the interfaces of the crack can be used as a crack detector 7. When the distance and the angular position of the crack detector 7 to the crack is kept constant independent from the glass thickness, it is also possible to deduce the crack depth or changes in the crack depth by way of the intensity or change in intensity of the measurement beam reflected back into the crack detector 7. The crack detector 7 could be fastened to the horizontally fixedly arranged shaft of a loose vertically movable roller which rolls in the edge area on the surface of the float glass ribbon 13. In this way, it maintains a constant distance from the crack and always directs its measurement beam at the same angle to the interfaces of the crack.
As soon as a crack is no longer detected, a signal is sent to the scribing device 10 which immediately initiates a new initial crack. The crack detector 7 can also supply a signal when the crack depth is not sufficient. The crack is made deeper by switching on another cooling nozzle 4.
Instead of the optical crack detector 7, the existing crack could also be verified by once again sensing the temperature subsequent to cooling. With knowledge of the heating temperature determined by the surface temperature immediately before the action of the laser beam, the given energy input by the laser and the temperature measured following the cooling, the generated temperature gradient can be deduced and therefore also the occurring tensile stresses which have generated a crack insofar as they have exceeded the breaking stresses. For this purpose, a second temperature sensor would be arranged following the final cooling nozzle 4.
The cutting process starts when an initial crack is made on the surface of the float glass ribbon 13 which is transported relative to the apparatus in the cutting direction identical to the drawing direction at a cutting speed identical to the drawing speed depending on the actual thickness of the float glass ribbon 13. In the cutting direction, starting with the initial crack, a specific depth crack is made in the float glass ribbon 13 comparable to a method according to U.S. Pat. No. 5,609,284 in that the float glass ribbon 13 is initially acted upon along the desired path of the crack by a laser beam having an elliptical beam cross section and is subsequently cooled. The float glass ribbon 13 is subsequently broken in a known manner along the crack that has been formed in this way.
Contrary to the teaching of U.S. Pat. No. 5,609,284 to adapt the beam geometry corresponding to thickness, the beam spot geometry, particularly the beam spot length, remains constant regardless of the thickness. In practice, a beam spot length of 120 mm, which corresponds to approximately ten-times the beam spot lengths indicated in the embodiment examples in U.S. Pat. No. 5,609,284, has proven successful for all standard thicknesses of the float glass ribbon 13.
The laser output is controlled in the method according to the invention only as a function of temperature independent of the change in thickness which can have the range of a power of ten anyway. The range of variation of the temperature of the float glass ribbon 13 directly before the action of the laser is between approximately 50° C. and 80° C. The possible temperature differences result from the material-specific and thickness-specific regime of the active cooling in the annealing oven and the passive cooling through the plant temperature which can vary appreciably particularly over the course of a year.
A laser with an output of 200 W is sufficient for an apparatus which can process the full spectrum of conventional float glass thicknesses. For float glass installations provided only for producing glass of smaller thickness, e.g., only up to 6 mm, a laser with a maximum output of 100 W would even be sufficient.
It will be apparent to a person skilled in the art that the invention is not limited to the particulars of the embodiment forms discussed above by way of example, but that the present invention can be embodied in other specific forms without departing from the scope of the invention as set forth in the appended claims.
Number | Date | Country | Kind |
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10 2006 024 825.2 | May 2006 | DE | national |