EP1405031A1 - Dispositif pour verifier et controler une vitre en verre simple, un element en verre isolant ou un verre feuillete - Google Patents
Dispositif pour verifier et controler une vitre en verre simple, un element en verre isolant ou un verre feuilleteInfo
- Publication number
- EP1405031A1 EP1405031A1 EP01955116A EP01955116A EP1405031A1 EP 1405031 A1 EP1405031 A1 EP 1405031A1 EP 01955116 A EP01955116 A EP 01955116A EP 01955116 A EP01955116 A EP 01955116A EP 1405031 A1 EP1405031 A1 EP 1405031A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- glass
- light
- laminate
- housing
- light source
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 239000011521 glass Substances 0.000 title claims abstract description 262
- 239000005340 laminated glass Substances 0.000 title claims abstract description 13
- 238000012360 testing method Methods 0.000 title abstract description 5
- 238000000576 coating method Methods 0.000 claims abstract description 23
- 230000003287 optical effect Effects 0.000 claims abstract description 13
- 230000005693 optoelectronics Effects 0.000 claims abstract description 12
- 238000011156 evaluation Methods 0.000 claims abstract description 9
- 230000010287 polarization Effects 0.000 claims description 35
- 239000011248 coating agent Substances 0.000 claims description 16
- 239000005001 laminate film Substances 0.000 claims description 15
- 238000003860 storage Methods 0.000 claims description 4
- 238000005259 measurement Methods 0.000 description 11
- 238000009826 distribution Methods 0.000 description 8
- 238000000034 method Methods 0.000 description 4
- 230000006870 function Effects 0.000 description 3
- 238000011161 development Methods 0.000 description 2
- 239000011888 foil Substances 0.000 description 2
- 238000005286 illumination Methods 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 230000008859 change Effects 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 230000001066 destructive effect Effects 0.000 description 1
- 238000009658 destructive testing Methods 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- 230000001795 light effect Effects 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000012029 structural testing Methods 0.000 description 1
- 239000005341 toughened glass Substances 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/02—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness
- G01B11/06—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material
- G01B11/0616—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material of coating
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B11/00—Measuring arrangements characterised by the use of optical techniques
- G01B11/02—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness
- G01B11/06—Measuring arrangements characterised by the use of optical techniques for measuring length, width or thickness for measuring thickness ; e.g. of sheet material
Definitions
- the invention relates to a device for checking and checking a single glass pane, an insulating glass element comprising two or more parallel glass panes, e.g. an insulating glass window, or a laminate glass, with a first light source, the optical axis of which can be brought into the reflection position with the single glass pane, the insulating glass element or the laminate glass, and an optical unit which is fixed relative to this, for determining the mutual distance of the individual -Glass pane, the insulating glass element or the laminate glass reflected parallel light rays.
- an insulating glass element comprising two or more parallel glass panes, e.g. an insulating glass window, or a laminate glass, with a first light source, the optical axis of which can be brought into the reflection position with the single glass pane, the insulating glass element or the laminate glass, and an optical unit which is fixed relative to this, for determining the mutual distance of the individual -Glass pane, the insulating glass element or the laminate glass reflected parallel
- the thickness of the glass panes of an insulating glass element is determined by laser triangulation, the mutual distances of the laser beams reflected from the glass panes being able to be measured using a scale.
- the measurement error caused by the unsharpness of the light points generated by the reflected light beams only enables a relatively imprecise determination of the thickness and distance of the insulating glass element.
- the presence of a coating on the glass panes cannot be determined in this known device.
- Another method of determining a coating on an insulating glass element is to measure it capacitively.
- this is only possible up to a certain thickness of the insulating glass element and the suitable measuring device must always rest on the coated pane of the insulating glass element, which is not always possible if it is on the outside of a building, for example.
- the object of the invention is therefore to provide a device of the type mentioned at the outset with which a non-destructive check of the position of coatings or laminate foils present on a single glass pane, the glass panes of the insulating glass element or within a laminate glass, and a thickness measurement of the Coating or the laminate film is possible.
- Another object is to make the device portable, easy to handle and safe to use.
- the optical unit for determining the mutual distance of the reflected light beams is formed by a spatially resolving optoelectronic detector which is connected to an evaluation device which determines the thickness of the individual from the distances and intensities of the reflected light beams - Glass pane, the thickness of the individual glass panes of the insulating glass element or the thickness of the layers of the laminate glass and their mutual distances and / or the presence and location of coatings applied to the individual glass pane or the individual glass panes of the insulating glass element or from one or several laminate films contained in the laminate glass.
- an opto-electronic detector enables an exact measurement of the mutual distance of the rays reflected from the individual glass pane, the insulating glass element or the laminate glass, since the intensity maxima can be determined from the intensity distribution of the reflected rays, which enables a very precise distance determination enable. With their help, the thickness of the glass panes and also the thickness of the laminate films can be determined.
- a transport device is arranged at a distance from the first light source, on which individual glass panes, insulating glass elements or laminate glasses can be moved, so that the individual glass pane, the insulating glass element or of the laminated glass the first light source reaches the reflection position and the reflected light rays strike the optoelectronic detector.
- the glass panes moved past at a defined distance can thus be measured and checked during their movement without having to stop.
- Another variant of the invention may consist in that the device is arranged in a housing which can be placed on one of the outer sides of the individual glass pane, the insulating glass element or laminate glass, with at least one first opening in the housing for the passage of the light source from the first emittable light beam and the light rays reflected by the single glass pane, the insulating glass element or the laminate glass is provided.
- glass panes already installed in window frames or in building parts can be checked to determine whether a coating or a laminate film is present on or in these.
- the housing can be placed on the outside of the glass pane and the measurement can then be carried out.
- the optoelectronic detector is formed from a CCD (Charge Coupled Device) element containing a plurality of image memory points, and that of the individual - Glass pane, light rays reflected from the insulating glass element or from the laminate glass strike the image memory points.
- CCD Charge Coupled Device
- the CCD element is designed as a CCD line in which the image memory points are linear along the longitudinal axis the CCD line are arranged, and that the longitudinal axis of the CCD line runs in the plane spanned by the reflected light beams.
- An advantageous embodiment of the invention for practical use and for the manufacture of the device according to the invention can consist in that the at least one first opening for the passage of the light beam emittable by the first light source and that of the individual glass pane, the insulating glass element or the laminate glass back-reflected light rays - in a known manner - is excluded in a housing wall on the underside of the housing, and that the optical axis of the first light source, preferably in an angular range of 45 ° to 60 °, with respect to the housing wall.
- a very compact design of the device according to the invention can be achieved according to a further variant of the invention in that the first light source is formed by a laser diode.
- the first wall opening is rectangular and that the CCD line is arranged along the longitudinal central axis of the first wall opening and offset in height from the housing wall forming the first wall opening.
- a further embodiment of the invention can consist in that the evaluation device is connected to a display device via which the number, the thickness, the mutual spacing of the parallel glass panes and the position of a coating which may be present on the front or rear side of the individual glass pane or the glass panes of the insulating glass element or the number and thickness of the laminate films of the laminate glass can be displayed.
- the display device enables a clear and quick representation of the measurement result.
- an interference filter is arranged at a distance in front of the CCD line, taking into account the angle of incidence of the reflected Radiation is only permeable to the wavelength of the light emitted by the first light source. In this way, practically only light with the wavelength emitted by the first light source can reach the optoelectronic detector, which enables a very precise determination of the intensity of the reflected rays.
- a further reduction in the influence of stray light can be achieved in that, according to a further embodiment of the invention, the thickness of the housing wall on the underside of the housing is greater than the opening width of a recessed wall opening for the passage of the reflected light rays. From outside the device according to the invention, the light incident obliquely onto the opening from the surroundings of the glass pane or the insulating glass element can thus largely be prevented from entering through the opening or the stray light is absorbed on the opening wall.
- the invention further relates to a device for checking and checking a single glass pane, an insulating glass element consisting of two or more parallel glass panes, e.g. an insulating glass window, or a laminate glass.
- the object of the invention is to provide a device of the aforementioned type which, in addition to determining the thickness of single and multiple (insulating) glass panes, also enables simple and convenient structural testing which does not require the viewer to perform tiring test steps.
- this is achieved in that a second light source for emitting a flat light field and a first light polarization device and a second light polarization device are provided, the first light polarization device polarizing the light emitted by the second light source and the second light polarization device the light reflected from the single glass pane, from the insulating glass element or from the laminated glass polarizes.
- the light field viewed under polarized light gives at a glance information about the structure that forms during glass hardening and thus the presence of hardened or unhardened glass panes.
- a transport device is arranged at a distance from the second light source, on which individual glass panes, insulating glass elements or laminate glasses can be moved, so that during the movement past the single glass pane, the insulating glass element or the laminate glass, the flat light field emittable by the second light source strikes the glass surface.
- the condition of the glass quality can be checked during the transport movement of the glass panes, the movement even being able to be used to move the entire surface of the glass with the device according to the invention.
- the observation of the reflected light can be automated.
- the device comprises a housing which can be placed on one of the outer sides of the individual glass pane, the insulating glass element or the laminate glass, that the housing has at least one second opening for the passage of the surface area which can be emitted by the second light source Luminous field and the first light polarization device is arranged in the region of the second light source, and that a housing window directed towards the second housing opening is provided, in the region of which a second light polarization device is arranged.
- the device housed in the housing can be placed on a built-in glass element and the condition of the glass surface can be fully assessed by moving the housing.
- a further embodiment of the invention can consist in that the second light source is formed by a, preferably U-shaped, fluorescent tube. In this way, a very uniform illumination of the light field striking the insulating glass element can be achieved.
- a variant of the invention that is technically simple to implement is that the first light polarization device is formed by a first pole filter and the second light polarization device is formed by a second pole filter.
- a very comfortable and clear control of an insulating glass element or a laminate glass for the viewer can be carried out in a further embodiment of the invention in that the housing window is recessed in an inclined angle, preferably 45 °, of the housing wall, and that the second pole Filter is embedded in a first frame part running parallel to the housing window.
- a second frame part for receiving the first pole filter is arranged in the interior of the housing
- the plane is preferably oriented at a right angle to the first frame part, so that the first and second frame parts extend like a roof over the second opening.
- a stable and symmetrical positioning of the light polarization devices within the housing is thereby achieved.
- a uniform polarization over the entire light field can be achieved according to a further embodiment of the invention in that the fluorescent tube extends parallel to the plane of the second frame part.
- Fig.l is a plan view of the housing of an embodiment of the device according to the invention.
- FIG. 2 shows a plan view of the opened housing according to Fig.l
- FIG. 3 shows a section AA through the housing according to Figure 2;
- FIG. 4 shows a section BB through the housing according to FIG. 2;
- FIG. 5 shows a schematic representation of the beam path through an insulating glass element and a further embodiment of the device according to the invention
- FIG. 6 shows a schematic representation of the intensity distribution of the rays reflected from a pane of an insulating glass element according to FIG. 5,
- FIG. 7 shows a schematic representation of the intensity distribution of the rays reflected by a coated insulating glass element
- FIG. 9 shows a schematic representation of a further embodiment of the device according to the invention.
- Fig. 1 to 4 show a device for checking and checking an insulating glass element 41, 42 consisting of two parallel glass panes, for example an insulating glass window, a laminated glass or a similar object made of glass, which can also comprise more than two parallel glass plates.
- the control of individual glass panes is also possible with this device.
- the condition of the insulating glass can be checked and checked after it has been manufactured or after it has been installed in buildings, for example to ensure that any coatings that may have been applied have been correctly applied to the glass panes, and whether the glass has actually been hardened and not uncured Glass at the manufacture of the insulating glass element has been used. It is also possible to check a laminate glass in which, for example, a laminate film is glued between two parallel glass panes and the presence of which can be determined using the device according to the invention.
- One embodiment of the device comprises a housing 1 which can be placed on one of the outer sides of the insulating glass element 41, 42 and a first light source 2, preferably a laser light source 2, arranged therein, from which a light beam 10 directed downwards can be emitted.
- a first light source 2 preferably a laser light source 2 arranged therein, from which a light beam 10 directed downwards can be emitted.
- two or more openings can also be provided as long as these do not hinder the passage of the emitted and the reflected light.
- the housing 1 has on its underside three support points, not shown in FIG. 3, which ensure that the light beam 10 strikes essentially in a normal plane to the glass panes of the insulating glass element 41, 42, even with a slightly curved glass pane 41, which is a prerequisite for the correct function of the device is.
- a spatially resolving, optoelectronic detector 3 is provided for determining the mutual distance of the reflected light beams 11, 12, 13, 14 and their intensity.
- the optoelectronic detector is preferably formed from a CCD (Charge Coupled Device) element 3 containing a plurality of image storage points 17 (FIG. 6), which is arranged within the housing 1 in such a way that the insulating glass element 41, 42 reflected light rays 11, 12, 13, 14 strike the image storage points 17.
- CCD Charge Coupled Device
- the device according to the invention can be used in particular for hardened, laminated, coated and colored glasses. It can be protected against improper start-up by another sensor, which determines whether there is a glass surface in the measuring range.
- the mode of operation of the device according to the invention is shown on the basis of the beam path shown in FIG. 5 through an insulating glass element formed from three parallel panes 41, 42, 43. In most cases, these are due to an inert gas filled gap separated from each other, whereby both reflection and refraction phenomena are observed when the emitted beam passes.
- the distance between two glass panes can also be filled with a laminate film.
- the device according to the invention can also be used with such insulating glass panes, provided that there is a change in the refractive index between two panes.
- the reflected beam 11 strikes the CCD element 3, which in the illustrated embodiments of the device according to the invention is designed as a CCD line 3, in which the image memory Points 17 are arranged linearly along the longitudinal axis of the CCD line 3, the longitudinal axis of the CCD line 3 running in the plane spanned by the reflected light beam 10 and the further reflected light beams 11, 12, 13, 14, 15, 16, so that they all hit CCD line 3 and can be registered there.
- a metallic coating 50 is applied to the rear of the glass pane 41, as is customary for insulating glass elements.
- the non-reflected portion of the light beam 10 is broken upon entry into the glass pane 41 in accordance with its refractive index and partially reflected again at the rear side of the glass pane 41, as a result of which a reflected light beam 12 parallel to the reflected light beam 11 emerges at the front side of the glass pane 41 and displaces it strikes the light beam 11 on the CCD line 3.
- the other glass panes 42, 43 generate in the same way on their front and back reflected beams 13, 14 and 15, 16, respectively, which strike the CCD line 3 offset from one another.
- the multiple refraction of the reflected rays caused by the other glass panes of the insulating glass element on the way to the CCD line 3 is shown in FIG. 5.
- the coating 50 on the back of the glass pane 41 increases the proportion of the light reflected by this coating 50 compared to a glass pane which is uncoated at this point.
- the resulting increase in intensity of the reflected beam 12 is reproduced in FIG. 7, in which the intensity I of the reflected light and incident on the CCD line 3 is plotted as a function of the distance x measured along the CCD line 3.
- the beam 11 reflected on the front of the glass pane 41 produces a first intensity distribution, the maximum In of which is smaller than the maximum I * 2 that reflected on the rear of the glass pane 41 and the coating 50 Intensity distribution is.
- the intensity maxima are at a distance from the glass thickness dl, which can thus be determined via the CCD line 3.
- the dashed line in FIG. 7 shows the intensity profile of an insulating glass element without coating 50.
- the lower light intensity reflected on the rear side of the glass pane 41 can be clearly seen in this case.
- the presence of a metallic coating can be determined from this difference in intensity.
- the light rays reflected on the second glass pane 42 are higher without coating 50 than with one. This must be taken into account when evaluating the measurement results.
- complicated cases with several coated glass panes or the simple case of a coated single glass pane can be dealt with in an analogous manner.
- the mutual distance a between the glass panes 41, 42 and the thickness d2 of the glass pane 42 can also be determined from the position of the intensity maxima.
- each image storage point 17 of the CCD line 3 being assigned a location coordinate.
- the spatial resolution is approximately 0.05 mm.
- the intensity distributions generated by the reflected rays 11 and 12 are resolved via the image memory points 17 of the CCD line 3 into discrete intensity measuring points, from which the position and the height of the maxima In and I ⁇ 2 can be determined.
- the distance between the maxima enables the thickness to be determined and the mutual distance between the glass plates to be determined.
- the CCD line 3 is connected to an evaluation device 45 (FIG. 5), which determines the presence from the intensities of the reflected light beams 11, 12, 13, 14, 15, 16 and the position of the coatings 50 applied to the individual glass panes of the insulating glass element 41, 42, 43 measured in FIG. 5 is determined.
- the evaluation device 45 is also connected to a display device 46, for example an LCD display, via which the number, the thickness, the mutual spacing of the parallel glass panes and the position of any coating, if any, on the front or back of the glass panes of the insulating glass. Elements 41, 42, 43 or one or more laminate foils contained in a laminate glass, optionally with the aid of graphic symbols.
- the display 46 is on the top of the Housing 1 attached, keys 21, 22 and 23 are provided for operating the device according to the invention (Fig.l).
- the first light source as a laser diode 2, e.g. to form red light, ⁇ 3 mW, the optical axis of which preferably extends at an angle of 45 ° to 60 °, preferably 52.5 °, relative to the housing wall 61.
- the first wall opening 60 for the passage of the light emitted by the laser diode 2 and reflected by the insulating glass element 41, 42 is rectangular in the exemplary embodiment shown.
- the CCD line 3 is arranged along the longitudinal central axis of the first wall opening 60 and offset in height from the housing wall 61 forming the first wall opening 60.
- an interference filter 67 is arranged - as seen in the direction of the reflected rays 11, 12, 13, 14 - at a distance in front of the CCD line 3, which only takes into account the angle of incidence of the reflected rays 11, 12, 13, 14 is transparent to the wavelength of the light emitted by the first light source 2. It can be inserted into the first opening 60.
- a further spectral filter 66 can be arranged in the beam path of the light emitted by the laser diode 2 before it is reflected by the insulating glass element.
- the thickness of the housing wall 61 on the underside of the housing 1 can be larger than the opening width of the opening 60 for the passage of the reflected light rays 11, 12, 13, 14, 15, 16. This limits the penetration of stray light. This is partially absorbed on the wall of the opening 60.
- a second light source 7 for emitting a flat light field and a first light polarization device 33 and a second light polarization device 32 are provided according to the invention , wherein the first light polarizing device 33 polarizes the light emitted by the second light source 7 and the second light polarizing device polarizes the light reflected from a single glass pane, from the insulating glass element 41, 42 or from a laminated glass.
- the housing 1 has a second opening 80 for the passage of the flat surface that can be emitted by the second light source 7 Luminous field and a housing window 38 directed towards the second housing opening 80.
- the second light source being formed by a, preferably U-shaped, fluorescent tube 7.
- the first light polarization device 33 is arranged in the area of the second light source 7 and the second light polarization device 32 in the area of the housing window 38, the first light polarization device 33 polarizing the light emitted by the second light source 7 and the second light polarization device that polarized light reflected by the insulating glass element 41, 42, wherein preferably a linear polarization of the light is carried out.
- a circular polarization would also be conceivable.
- Tempered glasses have a characteristic appearance when viewed under polarized light compared to unhardened glasses. When the area of the insulating glass element 41, 42 illuminated by the luminous field of the light source 7 is viewed, it can therefore be immediately judged whether a hardened or an uncured glass is present.
- the first light polarization device is preferably formed by a first pole filter 33 and the second light polarization device is formed by a second pole filter 32.
- the housing window 38 is recessed in a housing wall 40 of the housing 1 set at an oblique angle, preferably 45 °, the second polarizing filter 32 being embedded in a first frame part 42 running parallel to the housing window 38. A viewer can thus very comfortably view the field on the insulating glass element 41, 42 through the oblique side of the housing 1 and through the second opening 80.
- a second frame part 41 is also arranged inside the housing 1, the plane of which is at a right angle to the first Frame part 42 is oriented so that the first and second frame parts 42, 41 extend roof-like over the second opening 80.
- the fluorescent tube 7 is arranged parallel to the plane of the second frame part 41.
- the second opening 80 is covered by a protective glass 82.
- the laminate glass consists e.g. from two glass plates 70, 72, between which a laminate film 71 is glued, which e.g. is only around a 1/10 mm thick and has only a slightly different refractive index than glass, which is why the intensity of the light rays reflected at the transition from glass to film is relatively small.
- the rays reflected on the front of the glass pane 70 and on the rear of the glass pane 72 result in an intensity distribution whose maxima In and I 1 are much higher than the intensity maxima I 12 , L 3 that at the front and Back of the middle laminate film 71 are reflected rays.
- the two last-mentioned maxima can only be separately detected in the case of a very strongly collimated laser beam, otherwise there is only a single maximum, from which, however, it can at least be concluded that a laminate film is present. If both intensity maxima can be resolved, the spacing d2 of the laminate film can be determined from their spacing in addition to the thickness determination d1, d3 of the two glass panes 70, 72.
- Fig. 9 shows a further embodiment of the device according to the invention, in which a transport device, here support rollers 90, is arranged at a distance from the first light source 2, on which individual glass panes, insulating glass elements 41, 42 or laminate glasses can be moved, so that during the Moving the individual glass pane, the insulating glass element or the laminate glass past the first light source 2, this or this reaches the reflection position and the reflected light rays strike the optoelectronic detector 3.
- a transport device here support rollers 90
- the second light source 7, the first light polarization device 33 and the second light polarization device 32 can also be arranged at a distance from the transport device 90.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Investigating Materials By The Use Of Optical Means Adapted For Particular Applications (AREA)
Abstract
L'invention concerne un dispositif permettant de vérifier et de contrôler une vitre en verre simple, un élément en verre isolant (41, 42, 43) comprenant deux vitres parallèles ou davantage ou un verre feuilleté (70, 71, 72). Ce dispositif comprend une première source lumineuse (2) dont l'axe optique peut être placé en position de réflexion avec l'objet à mesurer et une unité optique pour déterminer l'écart mutuel des rayons lumineux (11, 12, 13, 14, 15, 16) parallèles réfléchis. L'unité optique est formée par un détecteur optoélectronique (3) à résolution locale, qui est relié à un dispositif d'évaluation (45) qui détermine sur la base des écarts et des intensités des rayons lumineux (11, 12, 13, 14, 15) réfléchis, l'épaisseur de la vitre en verre simple, celle des vitres en verre simples de l'élément en verre isolant (41, 42, 43) ou celle des couches du verre feuilleté(70, 71, 72) et leurs écarts mutuels et/ou la présence et la position de revêtement (50) appliqués sur la vitre en verre simple ou les vitres en verre simples de l'élément en verre isolant (41, 42, 43) ou d'une pellicule ou de plusieurs pellicules feuilletées (71) contenues dans le verre feuilleté (70, 71, 72).
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AT0181600A AT410257B (de) | 2000-10-23 | 2000-10-23 | Vorrichtung zur überprüfung und kontrolle einer einzel-glasscheibe oder eines isolierglas-elements |
AT18162000 | 2000-10-23 | ||
PCT/AT2001/000252 WO2002035181A1 (fr) | 2000-10-23 | 2001-07-23 | Dispositif pour verifier et controler une vitre en verre simple, un element en verre isolant ou un verre feuillete |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1405031A1 true EP1405031A1 (fr) | 2004-04-07 |
Family
ID=3689030
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP01955116A Withdrawn EP1405031A1 (fr) | 2000-10-23 | 2001-07-23 | Dispositif pour verifier et controler une vitre en verre simple, un element en verre isolant ou un verre feuillete |
Country Status (5)
Country | Link |
---|---|
US (1) | US20040099823A1 (fr) |
EP (1) | EP1405031A1 (fr) |
AT (1) | AT410257B (fr) |
AU (1) | AU2001277383A1 (fr) |
WO (1) | WO2002035181A1 (fr) |
Families Citing this family (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2846421B1 (fr) * | 2002-10-23 | 2004-12-17 | Saint Gobain | Procede de detection de couches minces tres faiblement visibles |
GB0419772D0 (en) * | 2004-09-07 | 2004-10-06 | Scalar Technologies Ltd | Method and apparatus for thin film metrology |
US7898524B2 (en) | 2005-06-30 | 2011-03-01 | Logitech Europe S.A. | Optical displacement detection over varied surfaces |
DE102006049946A1 (de) * | 2006-10-19 | 2008-04-24 | Boraglas Gmbh | Verfahren und Sensoranordnung zur Untersuchung von Glasscheiben, insbesondere wenigstens eines Glasscheibenstapels |
FI20095794A0 (fi) * | 2009-07-16 | 2009-07-16 | Sparklike Ab Oy | Menetelmä ja järjestelmä heijastavan läpinäkyvän kohteen ominaisuuksien tarkastelemiseksi |
US9109879B2 (en) | 2012-02-29 | 2015-08-18 | Corning Incorporated | Systems for and methods of characterizing the thickness profile of laminated glass structures |
US8895941B2 (en) | 2012-02-29 | 2014-11-25 | Corning Incorporated | Laminated glass sheet depth profile determination |
TWI700473B (zh) | 2014-06-04 | 2020-08-01 | 美商康寧公司 | 用於量測玻璃物品厚度的方法及系統 |
US10594920B2 (en) * | 2016-06-15 | 2020-03-17 | Stmicroelectronics, Inc. | Glass detection with time of flight sensor |
TWI804401B (zh) | 2022-07-28 | 2023-06-01 | 國立成功大學 | 光學量測系統 |
Family Cites Families (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3807870A (en) * | 1972-05-22 | 1974-04-30 | G Kalman | Apparatus for measuring the distance between surfaces of transparent material |
GB8611728D0 (en) * | 1986-05-14 | 1986-06-25 | Tole W R | Determining thickness of glass plates & tubes |
DE3926349A1 (de) * | 1989-08-09 | 1991-02-14 | Sick Optik Elektronik Erwin | Optische fehlerinspektionsvorrichtung |
DE19545369C1 (de) * | 1995-12-05 | 1997-04-03 | Fraunhofer Ges Forschung | Verfahren und Vorrichtung zur Abstands- und Profilmessung |
FR2751068B1 (fr) * | 1996-07-09 | 1998-10-30 | Lasers Et Tech Avancees Bureau | Dispositif optique de mesure a distance d'epaisseur de verre |
DE19758214A1 (de) * | 1997-12-31 | 1999-07-01 | Burkhard Dipl Ing Huhnke | Optische Präzisionsmeßeinrichtung zur Bestimmung der Kantenposition, der Kantensteigung und der Rauhigkeitskenngrößen von unbewegten, sowie zur Bestimmung des Durchmessers, der Kreis- und Zylinderformabweichungen bei bewegten rotationssymmetrischen Werkstücken während des Fertigungsprozesses, indem das im Abstandssensor durch Laserbeleuchtung von Objektkanten entstehende zweidimensionale Fresnel'sche Beugungsbild nach Steigung, Dämpfung der Einhüllenden, der Ortsfrequenz und nach Höhenschichtlinien ausgewertet wird |
DE19805200B4 (de) * | 1998-02-10 | 2006-02-09 | Micro-Optronic-Messtechnik Gmbh | Auswerteverfahren für eine Dickenmessung an Objekten |
US5966214A (en) * | 1998-05-12 | 1999-10-12 | Electronic Design To Market, Inc. | Gauge for measuring glass thickness and glass pane spacing |
US6285451B1 (en) * | 1999-04-30 | 2001-09-04 | John M. Herron | Noncontacting optical method for determining thickness and related apparatus |
-
2000
- 2000-10-23 AT AT0181600A patent/AT410257B/de not_active IP Right Cessation
-
2001
- 2001-07-23 AU AU2001277383A patent/AU2001277383A1/en not_active Abandoned
- 2001-07-23 WO PCT/AT2001/000252 patent/WO2002035181A1/fr not_active Application Discontinuation
- 2001-07-23 US US10/399,815 patent/US20040099823A1/en not_active Abandoned
- 2001-07-23 EP EP01955116A patent/EP1405031A1/fr not_active Withdrawn
Non-Patent Citations (1)
Title |
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See references of WO0235181A1 * |
Also Published As
Publication number | Publication date |
---|---|
ATA18162000A (de) | 2002-07-15 |
AU2001277383A1 (en) | 2002-05-06 |
WO2002035181A1 (fr) | 2002-05-02 |
AT410257B (de) | 2003-03-25 |
US20040099823A1 (en) | 2004-05-27 |
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