EP2828571B1 - Projektionsmodul für ein kraftfahrzeug - Google Patents
Projektionsmodul für ein kraftfahrzeug Download PDFInfo
- Publication number
- EP2828571B1 EP2828571B1 EP13716173.3A EP13716173A EP2828571B1 EP 2828571 B1 EP2828571 B1 EP 2828571B1 EP 13716173 A EP13716173 A EP 13716173A EP 2828571 B1 EP2828571 B1 EP 2828571B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- light
- reflector
- light source
- reflecting surface
- lens
- 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.)
- Active
Links
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- 239000003518 caustics Substances 0.000 description 12
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- 230000007423 decrease Effects 0.000 description 3
- 238000005286 illumination Methods 0.000 description 3
- 238000009434 installation Methods 0.000 description 3
- 230000004075 alteration Effects 0.000 description 2
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Images
Classifications
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21S—NON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
- F21S41/00—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
- F21S41/10—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by the light source
- F21S41/14—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by the light source characterised by the type of light source
- F21S41/141—Light emitting diodes [LED]
- F21S41/147—Light emitting diodes [LED] the main emission direction of the LED being angled to the optical axis of the illuminating device
- F21S41/148—Light emitting diodes [LED] the main emission direction of the LED being angled to the optical axis of the illuminating device the main emission direction of the LED being perpendicular to the optical axis
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21S—NON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
- F21S41/00—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
- F21S41/20—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by refractors, transparent cover plates, light guides or filters
- F21S41/25—Projection lenses
- F21S41/26—Elongated lenses
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21S—NON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
- F21S41/00—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
- F21S41/30—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by reflectors
- F21S41/32—Optical layout thereof
- F21S41/323—Optical layout thereof the reflector having two perpendicular cross sections having regular geometrical curves of a distinct nature
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21S—NON-PORTABLE LIGHTING DEVICES; SYSTEMS THEREOF; VEHICLE LIGHTING DEVICES SPECIALLY ADAPTED FOR VEHICLE EXTERIORS
- F21S41/00—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps
- F21S41/30—Illuminating devices specially adapted for vehicle exteriors, e.g. headlamps characterised by reflectors
- F21S41/32—Optical layout thereof
- F21S41/33—Multi-surface reflectors, e.g. reflectors with facets or reflectors with portions of different curvature
- F21S41/338—Multi-surface reflectors, e.g. reflectors with facets or reflectors with portions of different curvature the reflector having surface portions added to its general concavity
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21W—INDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
- F21W2102/00—Exterior vehicle lighting devices for illuminating purposes
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21W—INDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
- F21W2102/00—Exterior vehicle lighting devices for illuminating purposes
- F21W2102/10—Arrangement or contour of the emitted light
- F21W2102/13—Arrangement or contour of the emitted light for high-beam region or low-beam region
- F21W2102/135—Arrangement or contour of the emitted light for high-beam region or low-beam region the light having cut-off lines, i.e. clear borderlines between emitted regions and dark regions
- F21W2102/155—Arrangement or contour of the emitted light for high-beam region or low-beam region the light having cut-off lines, i.e. clear borderlines between emitted regions and dark regions having inclined and horizontal cutoff lines
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21W—INDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO USES OR APPLICATIONS OF LIGHTING DEVICES OR SYSTEMS
- F21W2102/00—Exterior vehicle lighting devices for illuminating purposes
- F21W2102/20—Illuminance distribution within the emitted light
Definitions
- the invention relates to a light module for a motor vehicle as from the generic document EP 1 225 388 known.
- the invention relates to a vehicle headlight with at least one such light module.
- the light module according to the invention is a projection system in which light from a light source is focused by a primary optics in the form of a reflector and directed onto a (projection) lens, which projects the desired light image onto an area in front of the light module or vehicle ,
- the reflector In contrast to a classic structure in which a real intermediate image is generated by the reflector, in the present invention, the reflector generates a virtual intermediate image of the light source, which then imaged by the lens in the form of a converging lens in the area in front of the light module or vehicle becomes.
- the reflector is designed as a hyperbolic reflector or essentially has the behavior of a hyperbolic reflector.
- the reflector in a first variant of the invention, provision is made for the reflector to be formed essentially as a reflector subshell, for example as a reflector half shell, to form the at least one light-dark line in the light image, and light from a region of the boundary edge of the reflector Reflector part shell forms the light distribution on the light-dark line in the photograph.
- the edge of the reflector acts as a hatch between the virtual object and the lens.
- portions of the reflector that are farther away from the lens have more of the character of a field of view diaphragm, a change of these areas also changes the imaged image section and accordingly these areas can be used to form the light image.
- the upper regions of the reflector can be trimmed in order to reduce the intensity of the light distribution in advance, while the trimming at the lower edge of the shape the light distribution on the HD line can be varied.
- the reflector sub-shell in the installation position of the light module is open at the bottom, so that there is a light-dark line in the overhead light.
- the boundary edge of the reflector partial shell extends substantially above a plane in which the at least one light source lies.
- the light-dark line in the photograph can be lowered, for example, by 0.57 ° (ECE control) or 0.4 ° (SAE control), as required for a law-compliant low beam distribution.
- the boundary edge is bent towards the front, to the front reflector opening towards the top.
- Curved "upwards” means primarily that the boundary edge of the plane in which the light source is located, bent away.
- the light source is inclined to a horizontal plane and the boundary edge is basically parallel to the inclined light source. The effect can occur that in an outer edge region of the light distribution, the light distribution is bent upward, so that light reaches an area above the legally permitted areas.
- the at least one light source has an elongated configuration, and that the light source is arranged with respect to the reflector that in the light image that of the reflective Surface of the reflector generated helical images are substantially parallel to the cut-off in the light image, since the extent of the blur is directly proportional to the size of a helical image, measured across the cut-off line.
- the longitudinal axis of the light source thus runs substantially parallel to the light-dark boundary to be generated, wherein an inclination of a few degrees with respect to the light-dark boundary may well be visually meaningful.
- such a light source has a significantly longer longitudinal than transverse extent, for example, it is a light source of a plurality of light emitting diodes, e.g. in a (1 x n) arrangement in which n LEDs are arranged in a row, the light source thus has a width of one LED and a length of n LEDs.
- elongated light sources are the arc of a Xe torch or the filament of an incandescent lamp.
- the at least one light source has a plane light exit surface, the light exit surface facing the reflective surface of the reflector.
- the light-emitting surface of the at least one light source is preferably substantially planar and wherein the boundary edge of the reflector forming the light-dark boundary is arranged in a region, in which the light-emitting surface of the at least one light source is shortened in perspective.
- This latter measure can be realized independently or together with the above-mentioned elongated embodiment of the light source.
- the reflector generates one or more light-dark boundaries in the light image by the reflector acts as a real aperture, so the boundary edge (s) of the reflector in the light image as light-dark boundaries (or areas of maximum brightness) be imaged.
- the reflecting surface of the reflector is embodied such that light from the at least one light source, which is reflected along at least one defined curve on the reflecting surface, is imaged in the light image as a region with maximum brightness.
- the generation of one or more light-dark boundaries with a reflector is based on the effect of the so-called caustics, so that one or more fundamentally arbitrarily shaped light-dark boundaries can be generated without the use of diaphragms.
- the at least one defined curve on the reflecting surface is displayed in the light image as a caustic line, ie as a line with maximum brightness, on one side (eg below this line) the brightness decreases, on the other side (eg above the line) no or hardly any light shown.
- the reflective surface of the reflector is formed such that light from both sides of the at least one defined curve on the reflective surface in the light image on one side of the area with maximum brightness, is subsequently imaged on this area.
- Such a reflector according to the invention can be varied flexibly, for example in order to make it smaller with regard to the installation space.
- this reflector is substantially parallel to the defined curve on the reflecting surface, which is imaged in the light image as an area with maximum brightness, on at least one side the defined curve is cropped.
- this reflector is trimmed substantially normal to the defined curve on the reflecting surface, which is imaged in the light image as a region with maximum brightness ,
- a designed as a real aperture reflector is provided with one or more defined curves which produce a Kaustikline, resulting in a variety of design options with regard to the generation of the light image.
- a light module according to the invention has the particular advantage that the total depth of the light module is no longer determined by the sum of the focal lengths of primary optics (reflector) and secondary optics (lens), but by the difference of the two focal lengths and thus can be greatly reduced theoretically. Even if practical limitations (finite size of the light source, manufacturing tolerances, etc.) are given, and thus the reduction of the installation depth limits are set, in a light module or headlight according to the invention the construction volume can be significantly lower than in conventional, known systems.
- the focal length per se is a quasi-free design parameter that can be used to improve the light image.
- the total refractive power is distributed to reflector and lens.
- the cross section of the lens is comparable to a classical projection system with a real intermediate image and otherwise similar characteristics, so that the required numerical aperture of the lens decreases. Since chromatic aberration occurs only in refraction, but not in reflection, can be achieved by the fact that a part of the refractive power is taken over by the reflector, already an improvement in color fidelity.
- the lens can be designed as achromatic, which is also useful for correcting chromatic aberrations.
- classical projection lenses with very large numerical aperture it is not possible to perform the lens as achromats.
- FIG. 1 schematically shows a light module 1 for a motor vehicle, comprising a light source 1, a reflector 2 and a lens.
- the reflecting surface 2a of the reflector 2 is shaped in such a way that a first focal point F1 of the reflector 2 lies between the reflecting surface 2a and the lens 3.
- a second focal point F2 lies on the side of the reflector 2 facing away from the lens 3, ie behind the reflector.
- the light emitted by the light source 1 is formed by the reflective surface 2a of the reflector 2 to a light distribution and - in the installed state of the light module 1 in a vehicle - is imaged via the lens 3 in an area in front of the vehicle.
- the light module 1 In the light module 1 according to the invention (and also in all other modules or systems shown) is a projection system in which light from a light source by a primary optics in the form of a reflector is focused and directed to a (projection) lens, which the desired light image is projected onto an area in front of the light module or vehicle.
- the reflector 2 In contrast to a classical construction in which a real intermediate image is generated by the reflector, in the present invention the reflector 2 generates a virtual intermediate image of the light source, which essentially comes to lie in the rear focal point F2 of the reflector 2, and becomes this intermediate image then imaged by the lens 3 in the form of a converging lens in the area in front of the light module or vehicle.
- the reflector is designed as a hyperbolic reflector or essentially has the behavior of a hyperbolic reflector, and the focal point of the lens 3 lies substantially in the rear focal point F2 of the reflector 2.
- FIG. 1 If you look at FIG. 1 , so you can see the areas bounded by arrows areas of the reflector 2. Cuts one in FIG. 1 illustrated reflector 2 above the area indicated by the arrow above and below the area marked with the arrow below, so only the two rays S1, S2 and intervening rays appear as the boundary rays from the reflector 2 and are imaged by the lens 3 ,
- Fundamentally inventive feature in a present light module is that the reflective surface of the reflector is formed such that the generated light image has at least one light-dark line.
- the edge of the reflector acts as a hatch between the virtual object and the lens.
- portions of the reflector that are farther away from the lens have more of the character of a field of view diaphragm, a change of these areas also changes the imaged image section and accordingly these areas can be used to form the light image.
- the upper regions of the reflector are trimmed to reduce the intensity of the light distribution in advance, while the trimming at the lower edge, the shape of the light distribution on the HD line varies can be.
- FIGS. 2 to 5 show a light module 1 with a light source 10, reflector 20 with reflective surface 20a and lens 30.
- the proportions are purely schematic, in particular, the lens can be significantly smaller and is for example as large as the reflector.
- the reflector 20 is designed as a partial shell, in particular as a half shell, and the light source 10 radiates light into this half shell, from which the light is reflected at the reflective surface 20a.
- the reflector half shell 20 is bounded by a boundary edge 20 ', 20 ", as shown in FIGS FIGS. 4 and 5 is shown.
- the boundary edge 20 ', 20 "in this example (after trimming, as will be described) lies in a horizontal plane, the light-dark boundary also essentially forms a horizontal straight line, as shown in FIGS FIGS. 6 and 7 easy to recognize.
- the boundary edge 20 ', 20 "of the reflector subshell 20 extends substantially above a plane in which the light source 10 lies, in this way the light / dark line in the light image can, for example as with a lawful low-beam distribution requested by 0.57 ° (ECE control) or 0.4 ° (SAE control) are lowered, as shown in the FIGS. 6 and 7 is shown.
- ECE control 0.57 °
- SAE control 0.4 °
- the light source 10 can, as this particular in FIG. 4 can be seen well, so that the plane in which the light source is inclined accordingly.
- the in the FIGS. 6 and 7 at about 5 ° lying asymmetry part is not formed by the edge 20 ', but is usually from one in the FIGS. 2 to 5 Not shown reflector segment, based on a segment 22 as in FIGS. 8 and 9 shown, generated.
- the at least one light source has an elongated configuration, and that the light source is arranged with respect to the reflector that in the light image that of the reflective Surface of the reflector generated helical images are substantially parallel to the cut-off in the light image, since the extent of the blur is directly proportional to the size of a helical image, measured across the cut-off line.
- the longitudinal axis of the light source thus runs substantially parallel to the light-dark boundary to be generated, wherein an inclination of a few degrees with respect to the light-dark boundary may well be visually meaningful.
- such a light source has a significantly longer longitudinal than transverse extent, for example, it is a light source of a plurality of light emitting diodes, e.g. in a (1 x n) arrangement in which n LEDs are arranged in a row, the light source thus has a width of one LED and a length of n LEDs.
- elongated light sources are the arc of a Xe torch or the filament of an incandescent lamp.
- the at least one light source has a plane light exit surface, the light exit surface facing the reflective surface of the reflector.
- the plane of the light source and the plane in which the lower boundary edge of the reflector lies extend in a substantially parallel plane.
- the light-emitting surface of the light source is preferably substantially planar and wherein the boundary edge of the reflector forming the cut-off line is arranged in a region in which the light-emitting surface of the at least one light source is shortened in perspective is.
- This latter measure can be realized independently or together with the above-mentioned elongated embodiment of the light source.
- the reflector generates one or more light-dark boundaries in the light image by the reflector acts as a real aperture, so the boundary edge (s) of the reflector in the light image as light-dark boundaries (or areas of maximum brightness) be imaged.
- FIGS. 8 and 9 show a light module 1 with a reflector 21, light source 11 and lens 31.
- the reflector 21 has a reflective surface 21a and a lower boundary edge 21 'comparable to that at the top of the hand FIGS. 2 to 5 described embodiment.
- the hyperbolic reflector has a focal length of about 40 mm
- the lens is an aspherical converging lens with a focal length of about 100 mm.
- the reflector 21 has an additional reflector region 22 with reflective surface 22a.
- This reflector region or this reflector segment 22 illuminates a central region directly around HV in the low beam distribution.
- this reflector segment 22 or its reflective surface 22a is designed such that it generates a so-called caustic.
- FIG. 10 schematically the reflective surface 22a, on which a plurality of reflector locations P1, P2, P3, P4, P5, P6 are highlighted.
- FIG. 11 shows the helical images W1 - W6 generated by these reflector locations P1 - P6 in the light image. If one wanders along the reflector along a line connecting the points P1-P6, then for the time being the helical images W1, W2, W3 travel with the corresponding points P1-P3.
- the point P3 represents an extreme position, ie a reversal point for the spirals in the light image, because we recognize, wander in a progression from P3 to P4 and then to P5 and P6, the coils W4, W5, W6 back towards the helix W1 ,
- the helical image W3 therefore touches the caustic with its outermost boundary edge W3 '(see below for further explanation), the reflector 22 or the reflector surface 22a can be trimmed in the vicinity of the point P3 without the sharpness of the cut-off change.
- FIG. 12 shows in the upper picture a light image, generated with an untrimmed reflector
- the lower figure in FIG. 12 shows the light image at a trimming of the reflector in the vicinity of those reflector locations, which correspond to helical images on the envelope of Kaustik, as to the hand FIGS. 10 and 11 described.
- the trimming results in the shape of the reflector 22.
- the trimming makes the light-dark boundary stand out better, in particular results in a better straight-line course of the oblique light-dark boundary, as in FIG. 12 easy to recognize.
- light module is the overall depth of about 70 mm.
- the lens was assumed to have a diameter of 100 mm, whereby the trimming can be made very flexible due to the beam path. Very small lens cuts (down to minimum sizes of 40mm x 30mm) are possible without having to sacrifice great efficiency losses.
- the example in the sketch shows a light exit area of 65mm x 45mm.
- a light source moved away from the lens is displayed higher.
- this closer LED row produces an upwardly shifted light distribution that can meet the legal requirements for a high beam distribution.
- the rear row of LEDs is thus shown lower in the focal plane of the lens than the front row.
- the multi-line LED light source can be rotated about an axis passing through the dimmed light relevant chips.
- the high beam row is intentionally defocused, resulting in a more homogeneous appearance and greater high beam height.
- FIG. 13 shows a light module 1 with a light source 100, a reflector 200 (with reflective surface 200a) and a lens 300, wherein the reflective surface 200a of the reflector 200 is formed such that light from the light source 100, which along a defined curve on the reflective Surface 200a is reflected in the light image as a region of maximum brightness.
- the light source 100 comprises one or more light-emitting diodes, which are arranged vertically, the light-emitting surface of which thus lies in a vertical plane, and this light source 100 illuminates the laterally arranged reflector 200, which generates a substantially horizontal light-dark boundary, as shown in FIG Photograph in FIG. 14 is shown.
- the HD limit is generated according to the invention exclusively by a caustic.
- the depth of the light module 1 is about 50 mm.
- the generation of the bright-dark boundary with a reflector is based here on the effect of the so-called caustics, so that one or more, in principle arbitrarily shaped light-dark boundaries can be generated without the use of diaphragms.
- the at least one defined curve on the reflecting surface is displayed in the light image as a caustic line, ie as a line with maximum brightness, on one side (eg below this line) the brightness decreases, on the other side (eg above the line) no or hardly any light shown.
- FIG. 15 shows a light module with a light source 110, in this case again comprising one or more vertically arranged LEDs, and this light source 110 illuminates a laterally arranged reflector 210 with reflective surface 210a. Via a lens 310, the light is projected into an area in front of the light module.
- a light source 110 in this case again comprising one or more vertically arranged LEDs, and this light source 110 illuminates a laterally arranged reflector 210 with reflective surface 210a. Via a lens 310, the light is projected into an area in front of the light module.
- This light module produces a semi-circular light distribution with a pronounced maximum, see FIG. 16 .
- the superposition with a mirror-image light distribution can be used to build a high beam.
- the essentially vertical cut-off line (see FIG. 16 ) is generated over the edge 210 'of the reflector 210.
- a basically hyperbolic reflector with, for example, a focal length of approximately 70 mm is used; in this example, furthermore, an aspherical converging lens with a focal length of approximately 90 mm is used.
- the depth of the light module is approximately 50 mm.
- FIGS. 17-20 the effect of the caustics, as in a partial reflector according to FIGS. 8 and 9 based on Figures 10 - 12 has already been briefly described, and how he also after a light module after FIG. 13 is used, will be described in more detail.
- FIG. 17 shows by way of example a laterally arranged reflector 2000 whose reflective surface 2000a is illuminated by a light source 1000.
- the reflecting surface 2000a of the reflector 2000 is designed according to the invention such that light from the light source 1000, which is reflected along the defined curve O on the reflecting surface 2000a, is imaged in the light image as a region with maximum brightness.
- light image illuminates light from an area around the line O in FIG. 17 a range at and below the horizontal cut-off line (see horizontal, hatched area LO in FIG. 18 ).
- the line O is substantially horizontal in this example.
- Light originating from the point 2 on the surface 2000a illuminates approximately the area marked "2" in the light image.
- FIG. 19 shows again the reflector 2000 with the reflective surface 2000a. Shown are three different vertically extending segments "A”, “B”, “C”, which represent the three areas “A”, “B”, “C” in the photograph in FIG FIG. 20 produce. Light from the area around the line O is imaged at the light-dark boundary, light from above and below the line O is imaged below the cut-off line.
- suitable segmentation and appropriate design of the individual segments which preferably connect continuously to each other, there is a great freedom of design with regard to the generation of a desired light image with cut-off.
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- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Geometry (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Optics & Photonics (AREA)
- Non-Portable Lighting Devices Or Systems Thereof (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
ATA50093/2012A AT512711B1 (de) | 2012-03-21 | 2012-03-21 | Lichtmodul für ein Kraftfahrzeug und Kraftfahrzeugscheinwerfer |
PCT/AT2013/050069 WO2013138834A1 (de) | 2012-03-21 | 2013-03-20 | Projektionsmodul für ein kraftfahrzeug |
Publications (2)
Publication Number | Publication Date |
---|---|
EP2828571A1 EP2828571A1 (de) | 2015-01-28 |
EP2828571B1 true EP2828571B1 (de) | 2016-06-22 |
Family
ID=48095450
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP13716173.3A Active EP2828571B1 (de) | 2012-03-21 | 2013-03-20 | Projektionsmodul für ein kraftfahrzeug |
Country Status (8)
Country | Link |
---|---|
US (1) | US9146013B2 (es) |
EP (1) | EP2828571B1 (es) |
JP (1) | JP5881887B2 (es) |
CN (1) | CN104204659B (es) |
AT (1) | AT512711B1 (es) |
IN (1) | IN2014MN02084A (es) |
MX (1) | MX2014011316A (es) |
WO (1) | WO2013138834A1 (es) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102015222363B4 (de) | 2015-08-27 | 2022-08-18 | Hyundai Motor Company | Lampenvorrichtung für fahrzeuge |
Families Citing this family (15)
Publication number | Priority date | Publication date | Assignee | Title |
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AT513816B1 (de) | 2012-12-20 | 2015-11-15 | Zizala Lichtsysteme Gmbh | Lichtführungseinheit für eine Leuchteinheit eines Scheinwerfers sowie Leuchteinheit und Schweinwerfer |
US10363860B2 (en) | 2013-12-12 | 2019-07-30 | Mitsubishi Electric Corporation | Headlight module and headlight apparatus |
WO2015191387A1 (en) | 2014-06-08 | 2015-12-17 | Valeo North America, Inc. | Lighting device with reflector and lens generating a light pattern with cutoff line |
JP6550788B2 (ja) * | 2015-02-23 | 2019-07-31 | 市光工業株式会社 | 車両用灯具 |
DE102015216746A1 (de) * | 2015-09-02 | 2017-03-02 | Volkswagen Aktiengesellschaft | Fahrzeugleuchte und Verfahren zum Bereitstellen einer Lichtfunktion mittels einer Fahrzeugleuchte |
AT517752B1 (de) * | 2015-09-17 | 2018-04-15 | Zkw Group Gmbh | Lichtmodul für einen kraftfahrzeugscheinwerfer zur abstrahlung einer langreichweitigen lichtverteilung sowie beleuchtungsvorrichtung |
DE112017000365B4 (de) * | 2016-01-13 | 2020-12-17 | Mitsubishi Electric Corporation | Scheinwerfermodul mit zwei bzw. drei reflektierenden Oberflächen und zwei gekrümmten Emissionsoberflächen, und Scheinwerfervorrichtung mit solch einem Scheinwerfermodul |
FR3048060B1 (fr) * | 2016-02-22 | 2019-04-05 | Valeo Vision | Dispositif de projection de faisceau lumineux muni de sous-matrices de sources de lumiere, module d'eclairage et projecteur muni d'un tel dispositif |
FR3048485B1 (fr) * | 2016-03-02 | 2019-04-05 | Valeo Vision | Lentille amelioree pour dispositif d'eclairage de vehicule automobile |
DE102016118152A1 (de) * | 2016-09-26 | 2018-03-29 | Automotive Lighting Reutlingen Gmbh | Lichtmodul für einen Kraftfahrzeugscheinwerfer |
CN110285381A (zh) * | 2018-03-19 | 2019-09-27 | 深圳市绎立锐光科技开发有限公司 | 一种光源模组以及车用前照灯 |
FR3084728B1 (fr) * | 2018-07-31 | 2021-03-19 | Valeo Vision | Module lumineux imageant la surface eclairee d'un collecteur |
JP2022502398A (ja) | 2018-09-27 | 2022-01-11 | 0903608 ビー シー リミテッド | 相乗的駆除組成物及び殺虫活性成分の送達方法 |
FR3130011B1 (fr) * | 2021-12-07 | 2024-04-05 | Valeo Vision | Dispositif lumineux d’un véhicule automobile |
FR3139375A1 (fr) * | 2022-09-06 | 2024-03-08 | Valeo Vision | Module d’éclairage route avec source lumineuse dirigée vers le haut |
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2013
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- 2013-03-20 US US14/386,578 patent/US9146013B2/en not_active Expired - Fee Related
- 2013-03-20 IN IN2084MUN2014 patent/IN2014MN02084A/en unknown
- 2013-03-20 WO PCT/AT2013/050069 patent/WO2013138834A1/de active Application Filing
- 2013-03-20 EP EP13716173.3A patent/EP2828571B1/de active Active
- 2013-03-20 CN CN201380015566.5A patent/CN104204659B/zh active Active
- 2013-03-20 MX MX2014011316A patent/MX2014011316A/es active IP Right Grant
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Also Published As
Publication number | Publication date |
---|---|
JP2015511057A (ja) | 2015-04-13 |
JP5881887B2 (ja) | 2016-03-09 |
US9146013B2 (en) | 2015-09-29 |
CN104204659B (zh) | 2017-06-13 |
WO2013138834A1 (de) | 2013-09-26 |
MX2014011316A (es) | 2014-10-17 |
IN2014MN02084A (es) | 2015-08-28 |
AT512711B1 (de) | 2014-08-15 |
CN104204659A (zh) | 2014-12-10 |
EP2828571A1 (de) | 2015-01-28 |
AT512711A1 (de) | 2013-10-15 |
US20150023045A1 (en) | 2015-01-22 |
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