• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a lighting device (1) for a headlight, in particular a motor vehicle headlight, comprising a plurality of light sources (100), a light guide device (10) having a plurality of light guide elements (11, 12, 13) and a downstream imaging optical element (200), wherein each light guide element (11, 12, 13) each has a light input surface and a respective light exit surface, wherein the light guide elements (11, 12, 13) are arranged in at least one row, wherein the light guide elements of at least one row as high beam light guide elements (11) each form a high-beam light guide element (11) each having a lower Lichtleitfläche (24), wherein the lower Lichtleitfläche (24) at least in that area in which the light beams (52) are reflected, at least partially structures (25 ) having.
    公开号:AT517523A1
    申请号:T50672/2015
    申请日:2015-07-28
    公开日:2017-02-15
    发明作者:Taudt Lukas；Plank Josef
    申请人:Zkw Group Gmbh；
    IPC主号:
    专利说明:

    Lighting device for a motor vehicle headlight
    The invention relates to a lighting device for a headlight, in particular a motor vehicle headlight, comprising a plurality of light sources, a light guide with a plurality of light guide elements and a downstream imaging optical element, each light guide each having a light input surface and a respective light exit surface, wherein the light guide in at least one row are arranged.
    Such lighting units, which are also referred to as pixel light modules, are common in the automotive industry and serve, for example, the imaging of glare-free high beam by the light is usually emitted by a plurality of artificial light sources and by a corresponding plurality of juxtaposed light guides (attachment optics / Primary optics) is focused in the emission direction. The light guides have a relatively small cross-section and therefore emit the light of the individual light sources each associated with very concentrated in the emission direction. Pixel light emitters are very flexible in terms of light distribution because for each pixel, i. For every light guide, the illuminance can be controlled individually and any light distribution can be realized.
    On the one hand, the concentrated radiation of the light guides is desired, for example, to comply with legal requirements regarding the light-dark line of a motor vehicle headlight or implement adaptive flexible Ausblendszenarien, on the other hand, this creates disturbing inhomogeneities in areas of the light image in which a uniform, concentrated and directed illumination desired is, as for example in the high beam distribution.
    This problem could be improved by reducing the height of the high beam distribution, which is in contradiction to customer requirements. There is therefore a need for improved measures for homogenizing the high beam distribution.
    Various measures or methods are known from the prior art, which are based on the one hand on the defocusing and on the other hand on the light scattering, for example by means of light-scattering structures.
    The US 8,011,803 B2 relates to a fog lamp, the collimating attachment optics with attached wavy deflection, which is inclined to the main emission of the LED includes. As a result, on the one hand, the light is deflected but also scattered, so that the homogeneity is improved.
    DE 2009 053 581 B3 relates to the primary optics of a matrix / pixel module. The frontal exit surface of the optic is provided with a wavy padding structure.
    DE 10 2008 005 488 A1 discloses a fine structure surface for the optical unit with a plurality of structural elements with which the light spots are widened in the horizontal direction. If the light spots overlap, the edges blur, resulting in a more homogeneous overall light distribution.
    DE 10 2010 027 322 A1 describes refractive micro-optic components on the light exit surface of a primary optic.
    EP 2 587 125 A2 discloses microstructures on the light exit surface of the primary optics of a pixel headlamp.
    US 5,727,108 discloses prismatic boundary surfaces for compound parabolic concentrator (CPC) alignment optics.
    It is an object of the invention to provide a lighting device for headlights, on the one hand allows a more homogeneous high beam distribution and on the other hand, a concentrated and directed illumination of a high beam area.
    This object is achieved with a lighting device for headlamps of the type mentioned, which is inventively characterized in that the light guide elements are formed at least one row as high beam light guide and form a high beam row, each high beam light guide each comprises a lower Lichtleitfläche, wherein the lower light guide surface at least in that area in which the light rays are reflected, at least in some areas having structures.
    The invention is a technically simple and cost-effective measure to locally influence the light distribution in the respective high-beam light guide elements and thus to realize a more homogeneous high beam distribution.
    The basic structure of light-guiding elements and attachment optics for pixel light lighting devices for headlights is known per se. The light-guiding elements are made, for example, of plastic, glass or any other suitable materials for light transmission. Preferably, the light guide elements are made of a silicone material. The light-guiding elements are typically embodied as solid bodies and preferably consist of a single continuous optical medium, wherein the light conduction takes place within this medium. The light-guiding elements typically have a substantially square or rectangular cross section and usually expand in the light emission direction in a manner known per se. In an alternative embodiment, the light-guiding elements can be realized as open collimators.
    Advantageously, the structures are formed in that region of the lower light guide surface which adjoins the light exit surface and in which the light is reflected. By arranging the structures only in the vicinity of the light exit surface of the respective high-beam light-guiding elements of the high-beam row, it is thus possible in particular to improve the superimposition of once-reflecting light beams on the directly emitted light.
    The light emitted by the light source and light coupled into the light guide is expediently totally reflected by the lower light guide surface.
    Advantageously, the structures formed on the lower light guide surface comprise structural elements which have a periodic geometry.
    It has been found that it is particularly advantageous if the structures are groove-shaped, wherein the grooves are oriented transversely to an optical axis of the lighting device.
    The grooves may have a width of about 0.2-0.4 mm and a height of 0.015-0.03 mm.
    In a variant, it is provided that, starting from the light exit surface, 6-15 grooves are formed on the lower light guide surface.
    Experience has shown that the structure of a lighting device for pixel light is particularly efficient when the light-guiding elements are arranged in exactly three rows arranged one above the other, which together form a high beam distribution. In such an arrangement, the upper row may be formed as a leading row, the middle row as an asymmetrical row and the lower row as a high beam row, the high beam row being provided by high beam light guiding elements having structures as described herein. Conveniently, the bottom row is the high beam row.
    In another embodiment, all the light-guiding elements can be designed as high-beam light-guiding elements which are arranged in exactly one row. Such lighting devices are also referred to as pixel high beam modules.
    The light-conducting elements of the rows are preferably arranged as close as possible to each other, whereby inhomogeneities in the photograph can be further reduced. In one development of the invention, the light exit surfaces of the individual light guide elements can therefore be part of a common light exit surface, with the individual light exit surfaces adjoining one another. The common light exit surface is typically a curved surface, usually following the Petzval surface of the imaging optics (e.g., an imaging lens). For certain applications, however, deliberate deviations in the curvature can also be used in order to use aberrations for light homogenization in the edge region.
    Another object of the invention relates to a headlamp, in particular a motor vehicle headlamp, which comprises a lighting device according to the invention as disclosed herein. Headlights of this type are also referred to as pixel light.
    The invention and its advantages are described in more detail below by way of non-limiting examples, which are illustrated in the accompanying drawings. The drawings show in:
    1 is a perspective view of the basic structure of a lighting device according to the invention,
    FIG. 2 is an illustration of the total light distribution obtained with the lighting device of FIG. 1. FIG.
    3 is a detail view of the optical attachment of Figure 1 in the light propagation direction,
    4 is a side view of a high-beam light guide according to the prior art,
    5 shows a light intensity distribution (light intensity simulation) of a high-beam light-conducting element from FIG. 4.
    6 shows an intensity curve of the light intensity distribution from FIG. 5, FIG.
    7 shows a side view of a high-beam light-conducting element according to the invention,
    8 shows a representation of the light intensity distribution of the high-beam light-conducting element from FIG. 7, FIG. 9 shows an intensity curve of the light intensity distribution from FIG. 8,
    10 shows a vertical section through a high-beam light-conducting element according to the invention, and FIG. 11 shows a detail from FIG. 10.
    Fig. 1 shows a perspective view of the basic structure of a lighting device 1 according to the invention. 1 comprises a plurality of LED light sources 100 not illustrated in detail in FIG. 1 (cf., however, FIG. 7) and an attachment optics 10 positioned in the light emission direction (= primary optics) and a downstream imaging optics 200 (shown as a single lens 200). , The attachment optics 10 comprises light-guiding elements 11, 12, 13, which are arranged in three rows and extend on the radiating side to a common end plate 26. The end plate 26 is the emission side limited by a light exit surface 23 ', wherein the light exit surfaces 23 of the individual light guide elements (see FIG. 7) each part of the common light exit surface 23', wherein individual light exit surfaces 23 adjacent to each other. The common light exit surface 23 'is typically a curved surface, usually following the Petzval surface of the imaging lens 200. For certain applications, deliberate deviations in the curvature of the common light exit surface 23 'can also be used in order to use aberrations for light homogenization in the edge region. Each light-guiding element 11, 12, 13 is associated with an LED light source 100 (see FIG. For each light guide element 11, 12, 13, the illuminance can be controlled individually, which is why arbitrary light distributions can be realized. In the optical attachment 10 shown in FIG. 1, the upper row is formed as a front row row consisting of a plurality of apron light-guiding elements 13. The middle row is formed as asymmetry series consisting of a plurality of asymmetry light guide elements 12 and the lower row is formed as a high beam row consisting of a plurality of high beam light-guiding elements 11. The three rows together form a high beam distribution in the activated state. The high-beam light-conducting elements 11 are provided on their lower light-guiding surface 24 (see FIG. 7) with a groove structure 25, wherein the grooves 25 are oriented transversely to an optical axis 16 of the lighting device 1. FIG. 3 shows a detailed view of the attachment optics 10 from FIG. 1 in the light propagation direction.
    The light-guiding elements 11, 12, 13 can be made, for example, of silicone, plastic, glass or any other suitable materials for light conduction. The light-guiding elements 11, 12, 13 are designed as solid bodies and consist of a single continuous optical medium, wherein the light conduit takes place within this medium. The light-guiding elements 11, 12, 13 have a substantially square or rectangular cross-section and extend in the direction of light emission, where they finally as described above radiation side to the common end plate 26, the emission side by a light exit plane 23 '(see Fig .. 3) limited is lost.
    2 shows a representation of the total light distribution (= pixel light distribution) with a view through the imaging lens on a measuring screen, which can be obtained with the lighting device 1 from FIG. It is about a horizontal axis U and a vertical
    Axis V matrix-shaped and arranged in three rows fields recognizable, the upper row, which includes a plurality of high beam strips, for illumination of the high beam area, the middle row for illumination in the asymmetry area (forming a cut-off) and the lower row for illumination the apron of a pixel light spotlight is used. Overall, the light distribution forms a high beam distribution. Adjacent fields touch or overlap each other, making the light image appear substantially homogeneous to a viewer.
    4 shows a side view of a high-beam light-conducting element 11 'according to the prior art. The high-beam light-conducting element 11 'is a solid body having a light coupling surface 21, via which the light emitted by the LED light source is coupled into the light-conducting element 11'. The light is conducted forward along the high-beam light-conducting element 11 'to a light exit surface 23. FIG. 4 also shows exemplary beam paths emanating from the light incoupling surface 21, wherein the beams 50 represent the direct light exit and the beams 51, which are reflected at a lower light guide surface 24, represent the indirect light exit. Also visible is the upper Lichtleitfläche 22, whereas the laterally limiting the solid body Lichtleitflächen speed reasons are not provided with reference numerals. The light rays are totally reflected at the light guide surfaces. 4, the lower light guide surface 24 of a prior art high-beam light guide element 11 'is formed along its entire length as a smooth reflection surface (optimized for the use of total reflection).
    5 shows, by way of example, a light intensity distribution 30 (photometric raytracing simulation with a light intensity sensor, a grayscale image being obtained in accordance with the luminous intensity) of a high-beam light-conducting element 11 'from FIG. 4. An intensity maximum 31 can be detected in the lower region of the high beam segment; In the upper area of the high beam segment, on the other hand, there is first an intensity drop 32, which leads to a clearly visible inhomogeneity due to a rise 33 of the intensity. FIG. 6 shows an intensity curve of the light intensity distribution from FIG. 5, in which the counter-rise 33 can be clearly seen. The cause of the inhomogeneity lies in particular in the transition and the insufficient overlap between the directly emitted light 50 and the light 51 reflected at the lower light guide surface 24.
    FIG. 7 shows a side view of a high-beam light-conducting element 11 according to the invention. The high-beam light guide element 11 according to the invention differs from that of the prior art (high-beam light guide 11 ', see Fig. 4) in that on the lower light guide surface 24 in that region in which the beams 52 are reflected, grooved Structures 25 are formed. The remaining structure of the high-beam light-guiding element 11 corresponds to that of FIG. 4 and reference is made to the description above. FIG. 7 also shows exemplary beam paths emanating from the light incoupling surface 21, wherein the beams 50 represent the direct light exit and the beams 52, which are reflected at the groove structure 25 of the light guide surface 24, represent the indirect light exit. The groove structure 25 scatters and shapes the light 52 precisely in that region which lies in the transition between the directly emitted light 50 and the light 52 reflected at the groove structure 25 of the lower light guide surface 24. By the groove structure 25, the light distribution can be influenced and as a result there is an improvement in the light homogeneity.
    8 shows by way of example a light intensity distribution 30 '(photometric raytracing simulation with a light intensity sensor, a grayscale image being obtained in accordance with the luminous intensity) of a high-beam light-conducting element 11 according to the invention from FIG. 7. The intensity maximum 31 can be detected in the lower area of the high beam segment ; In the upper part of the high beam segment, a continuous drop in intensity is generally recognizable and the light image is much more homogeneous compared to the prior art. FIG. 9 shows a intensity distribution curve of the light intensity distribution from FIG. 8, from which the continuous intensity drop and the improved homogeneity (marked with the reference symbol 34 in FIG. 7) in the transition between the directly emitted light 50 and the light 52 reflected at the groove structure 25 is clearly visible. With the aid of the groove structure, the outlet can be better designed or optimized (see FIG.
    10 shows a vertical section through a high-beam light-conducting element 11 according to the invention. As can be seen therein, the grooves 25 extend transversely to the optical axis (or light propagation direction) and are formed along a (imaginary) carrier curve TK on the lower light guide surface 24. In the example shown, a total of 9 grooves are formed starting from the light exit surface 23. For example, the grooves 25 have a width of 0.3 mm and a height of 0.015-0.03 mm.
    FIG. 11 shows a detail of FIG. 10 (indicated by a dashed circle in FIG. 10). An optimized embodiment can be obtained as follows: The support curve TK is the limitation of a light guide. On this curved (imaginary) curve TK points P (Pi, Pi + 1, Pi + 2) are plotted, which have a constant distance S from each other. This distance (or wavelength) is for a special high-beam light guide, for example, S = 0.30 mm. Neighboring Points Pi and Pi + 1 determine a path into whose halving point Hi a normal is established. Above the point, a vertex Si is established at a distance = amplitude of hi. The three points Pi, Si, Pi + 1 are the nodes of a spline curve. The magnitude of the amplitude is iteratively varied, with the respective geometry a photometric simulation is carried out according to a conventional manner. By comparing the obtained light images (or the gradient curve), the best amplitude is determined. This process must be repeated for each groove, since the distance from the light source (LED light source 100) determines the angle of incidence on the support curve and thus the position of the inhomogeneity. The boundary surface of the groove itself is an extension surface of the determined spline curve, wherein the extension direction is normal to the vertical center plane of the light guide, and wherein each groove has its own amplitude.
    The examples shown are only a few among many and not to be construed as limiting.
    权利要求:
    Claims (12)
    [1]
    claims
    A lighting device (1) for a headlamp, in particular a motor vehicle headlamp, comprising a plurality of light sources (100), a light guide (10) having a plurality of light guide elements (11, 12, 13) and a downstream imaging optical element (200), each Light guide element (11, 12, 13) each have a light input surface and each having a light exit surface, wherein the light guide elements (11,12,13) are arranged in at least one row, characterized in that the light guide elements at least one row as high beam light guide elements (11) are formed and form a high beam row, wherein each high-beam light guide element (11) each comprise a lower Lichtleitfläche (24), wherein the lower Lichtleitfläche (24) at least in that area in which the light beams (52) are reflected, at least partially structures ( 25).
    [2]
    2. Lighting device according to claim 1, characterized in that the structures (25) in that region of the lower light guide surface (24) which is adjacent to the light exit surface (23) and in which the light is reflected, are formed.
    [3]
    3. Lighting device according to claim 1 or 2, characterized in that the lower light guide surface (24) totally reflects the injected light beams.
    [4]
    4. Lighting device according to one of claims 1 to 3, characterized in that the structures comprise structural elements (25) which have a periodic geometry.
    [5]
    5. Lighting device according to one of claims 1 to 4, characterized in that the structures are groove-shaped, wherein the grooves (25) are oriented transversely to an optical axis (16) of the lighting device.
    [6]
    6. Lighting device according to claim 5, characterized in that the grooves (25) have a width of 0.2 - 0.4 mm and a height of 0.015 - 0.03 mm.
    [7]
    7. Lighting device according to claim 2 and 6, characterized in that, starting from the light exit surface, 6-15 grooves (25) on the lower light guide surface (24) are formed.
    [8]
    8. Lighting device according to one of claims 1 to 7, characterized in that the light-guiding elements (11, 12, 13) are arranged in exactly three rows arranged one above the other, which together form a high beam distribution.
    [9]
    9. Lighting device according to claim 8, characterized in that the bottom row (11) is the high beam row.
    [10]
    10. Lighting device according to one of claims 1 to 7, characterized in that all the light-guiding elements are designed as high-beam light-guiding elements, which are arranged in exactly one row.
    [11]
    11. Lighting device according to one of claims 1 to 10, characterized in that the light exit surfaces (23) of the light guide elements (11, 12, 13) are part of a common light exit surface (23 '), wherein individual light exit surfaces (23) adjoin one another.
    [12]
    12. A motor vehicle headlamp comprising a lighting device (1) according to one of claims 1 to 11.
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    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA50672/2015A|AT517523B1|2015-07-28|2015-07-28|Lighting device for a motor vehicle headlight|ATA50672/2015A| AT517523B1|2015-07-28|2015-07-28|Lighting device for a motor vehicle headlight|
    CN201680042909.0A| CN107850282B|2015-07-28|2016-07-18|Lighting mechanism and motor vehicle headlight|
    JP2017567754A| JP6481054B2|2015-07-28|2016-07-18|Lighting equipment for automotive headlamps|
    PCT/AT2016/060008| WO2017015684A1|2015-07-28|2016-07-18|Lighting device for a motor vehicle headlamp|
    EP16750359.8A| EP3329179B1|2015-07-28|2016-07-18|Light device for a vehicle headlamp|
    US15/564,372| US10018317B2|2015-07-28|2016-07-18|Lighting device for a motor vehicle headlamp|
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