• 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 collimator (200) has an overall shape of a bowl, the collimator (200) comprises a symmetry of revolution about an optical axis (5) of the collimator (200), an exit wall (4), an entry recess (6) opposite the exit wall (4), the inlet recess (6) being defined by an inner side wall (2) and an inner top wall (7) intersecting the inner side wall (2) so as to defining an intersection zone (8), the inner lateral wall (2) and the inner upper wall (7) being intended for the peripheral and central entrance respectively of a light beam incident in the collimator (200), a peripheral reflection wall (3) joining the outlet wall (4) to the inner side wall (2), the surface of the inner side wall (2) being configured so that a line (D) tangential to the side wall internal (2) and joining the intersection zone (8) passes through the focus (1) of the collimator (200).
    公开号:FR3019314A1
    申请号:FR1452747
    申请日:2014-03-28
    公开日:2015-10-02
    发明作者:Jean Pierre Lauret
    申请人:Gaggione Sas；
    IPC主号:
    专利说明:

    [0001] The present invention relates to an optical collimator for collimating a beam from a light source to limit Fresnel losses. In conventional collimators, the incident beams are transmitted by refraction through an entrance surface. This entrance surface is an optical surface separating two different refractive index materials. As a result, a portion of the incident beam is reflected by the collimator input surface instead of being transmitted, which constitutes Fresnel losses by reflection. For common optical materials, this portion reduces the overall light transmission by about 4%. This beam portion is then reflected by an outer reflection surface of the collimator and is transmitted at a high angle to the optical axis by an exit surface of the collimator. Thus, this beam portion then forms a parasitic peripheral ring around the main light beam coming from the collimation of the incident light beam. This decreases the quality of the resulting illumination, which in this way is not suitable for all desired applications, including applications in the medical field. A collimator for overcoming at least one of these disadvantages is therefore desirable. For this purpose, the present invention provides an optical collimator for collimating a beam from a light source, the collimator 20 having an overall shape of a bowl, the collimator comprising a symmetry of revolution about the optical axis of the collimator, a outlet wall, an inlet recess opposite to the outlet wall, the inlet recess being defined by an inner side wall and an inner top wall contiguous to the inner side wall so as to define an intersection zone, the inner side wall and the upper inner wall being intended for the entry, respectively peripheral and central, of a light beam incident in the collimator, a peripheral reflection wall joining the outlet wall to the inner side wall, the surface of the inner sidewall being configured so that a straight line D tangent to the inner side wall and joining the intersection area not stand by the focus of the collimator. Thus, in this configuration, the incident rays which would have been responsible for the formation of a parasitic peripheral ring are reflected on the inner side wall at grazing incidence. As a result, the reflection of these rays allows refocusing to the inner upper wall where they are collected as if they originated from a beam from a point near the focus. The refocused rays then add to the main beam which is brighter. Moreover, the parasitic annular ring is greatly reduced.
    [0002] It is understood in this document that the inner side wall and the inner upper wall are intended for the entry of incident light rays, the peripheral reflection wall is intended to reflect the rays intercepted by the inner side wall and the exit wall. is intended to bring out the light rays. Of course, throughout the document, the peripheral reflection wall is mutually configured with the inner sidewall so as to collimate an incident light beam. Advantageously, the inner side wall has a curvilinear surface 10 with symmetry of revolution around the optical axis of the collimator. Preferably, the inner side wall comprises a convex portion configured to intercept at the same point A a central radius from the focus and a virtual marginal radius extending a real marginal radius from the periphery of the light source, the actual marginal radius being intercepted at a point B of the inner sidewall and so that the peripheral reflection wall reflects the central radius at a point A 'and the actual marginal radius at a point B' with the distinct point A of the point B and the point A 'having a distance from the focus greater than that of the point B'. With this configuration, the actual marginal radius is intercepted earlier in its path by the inner sidewall which refracts it to the peripheral reflection wall. It then emerges from the output wall by being collimated, that is to say substantially parallel to the optical axis. The path of the real marginal radius is then substantially identical to that of a central ray coming from a point close to the focus. This configuration of the collimator thus makes it possible to collimate light rays quite far from the fireplace without necessarily having to extend the internal reflection wall. In the prior art, in fact, it is known to extend the internal reflection wall to intercept light rays coming from points distant from the focus. But this solution has the effect of moving the collimator design away from its ideal conformation and making it larger. Thus, the present invention makes it possible to collimate light sources that are larger than those that can be collimated by collimators of conventional configuration. Preferably, the inner sidewall comprises an annular zone defined from the focus at a solid angle α (alpha) between 35 ° and 90 ° with respect to the optical axis, the tangent of the annular zone forming an angle θ (beta ) Between 0 ° and 30 ° with respect to the optical axis. This annular zone thus has a relatively low slope allowing this zone of the inner side wall to be closer to the light source. This allows to illuminate a larger area in the vicinity of the collimator output surface. According to the law of conservation of the geometrical extent which says that the light beam is all the more intense as its section is large, this configuration thus makes it possible to obtain a more intense beam of light. Advantageously, the collimator is monobloc. Its manufacture therefore does not require assembly step between several parts, which reduces the labor and thus reduce costs. Preferably, the collimator is made of polymer which allows for molding production. Preferably, the polymer is a silicone. The flexibility of the silicone allows easy demolding of the collimator despite its design comprising a convex region forming an undercut. According to one possibility, the inner upper wall comprises a portion 15 having a convex surface. This conformation is conventionally calculated so as to transmit a majority of incident rays to the exit wall forming a collimated beam. According to yet another possibility, the outlet wall comprises a portion having a substantially flat surface. It is thus possible to focus the light to infinity. In a variant, the outlet wall comprises a portion having a substantially concave surface. This variant is particularly advantageous on collimators large dimensions because it allows a significant material gain. According to another variant, the outlet wall comprises a portion having a substantially convex surface, so as to converge the light rays coming from the hearth. This configuration thus makes it possible to focus the light in the near field. According to yet another variant, the exit wall is shared between a central zone and a peripheral zone, the central zone surface being configured to share the refraction of the incident light beam with the inner top wall so as to obtain a collimated beam. and the surface of the peripheral area being configured to operate in association with the peripheral reflection wall. These configurations make it possible to add degrees of freedom to the optical design of the collimator. This configuration of the surface of the central zone makes it possible to optimize more finely the light intensity distribution. The configuration of the surface of the peripheral zone may also be concave, convex or textured for example to improve its ability to converge, diverge light rays, etc. Advantageously, the central zone has a circle-shaped periphery and the peripheral zone has an annular shape delimiting the periphery of the central zone. According to one possibility, the exit wall has a surface comprising microtexturing configured to generate a type of light beam from the light source such as an intermediate beam, a wide beam, or an elliptical beam. It is thus possible to obtain different light intensity distributions from an intensive beam which is the base beam without microtexturing. The basic intensive beam will be for example 10 ° FWHM (full width half maximum), the intermediate beam to reach about 25 ° FWHM, the broad beam to reach about 40 ° FWHM and the elliptical beam 15 allowing to reach about 10 ° x40 ° FWHM. Other aspects, objects and advantages of the present invention will appear better on reading the following description of various embodiments thereof, given by way of non-limiting examples and with reference to the accompanying drawings. The figures do not necessarily respect the scale of all the elements shown so as to improve their readability. In the remainder of the description, for the sake of simplification, identical, similar or equivalent elements of the various embodiments bear the same numerical references. - Figures 1 and 2 show a known classic collimator type "flat top tulip". FIGS. 3 and 4 show a collimator according to a first embodiment according to the invention. FIG. 5 illustrates an annular zone of the collimator illustrated in FIGS. 3 and 4. FIG. 6 illustrates a collimator according to a second embodiment according to the invention. FIG. 7 illustrates a collimator according to a third embodiment according to the invention. FIG. 1 illustrates the path of an incident beam in a conventional optical collimator 100. A portion of the beam originating from the focus 1 of the collimator 100 is first refracted on an internal input side wall 2 forming a main beam. which is then reflected on a peripheral reflection wall 3 to emerge from an outlet wall 4 substantially parallel to the optical axis 5 of the collimator 100. The other part of the incident beam is reflected by the input wall 2 lateral following Fresnel reflection. This gives rise to a parasitic beam p which emerges from the outlet wall 4 at a high angle relative to the optical axis 5. This parasitic reflection or loss of Fresnel contributes to reducing the overall light output to approximately 4%. The parasitic beam p is also at the origin of a parasitic light ring around the main beam i collimated (not shown). FIG. 2 illustrates the path of an incident beam originating from the periphery of a light source, it is therefore remote from the focus 1 of the conventional collimator 100. This path is compared with the path of a beam i from the focus 1 which emerges from the outlet wall 4 along an axis parallel to the optical axis 5 and which is perfectly collimated. As illustrated in Figure 2, the far-away beam is not efficiently collected. The remote beam e passes through the inner side wall 2 and the outlet wall 4 without being focused on the peripheral reflection wall 3 because the latter is not large enough to be able to intercept it. Indeed, if the peripheral reflection wall 3 were prolonged, it would intercept the distant beam e before it reaches the exit wall 4. As a result, as shown in FIG. 2, the beam e emerges from the collimator 100 by being reflected by the outlet wall 4 and forming a high angle with the optical axis 5, in contrast to the beam i from the hearth 1 which is intercepted by the peripheral reflection wall 3 with an angle allowing a transmission through the wall 4. The beam e from the edge of the source is therefore at the origin, according to the architecture of the collimator 100, a loss of light intensity or parasitic light formation. Figure 3 is a collimator 200 according to a first embodiment of the invention. This collimator 200 comprises an overall shape of a bowl with a symmetry of revolution about its optical axis 5. The collimator 200 comprises an outlet wall 4, an inlet recess 6 opposite the outlet wall 4 and a peripheral reflection wall 3 joining the outlet wall 4 to the inlet recess 6. The outlet wall 4 allows the transmission of substantially collimated rays out of the collimator 200. This outlet wall 4 is flat but according to variants not shown, the wall of Exit 4 comprises a portion whose surface is convex or concave. According to another possibility, the surface of the outlet wall 4 comprises micro-texturing.
    [0003] The input recess 6 of the collimator 200 is intended for the input of the incident beams coming from the light source. It is composed of an inner side wall 2, whose surface is curvilinear while retaining the symmetry around the optical axis 5, and an inner top wall 7 comprising a convex surface portion. The focus 1 of the collimator 200 is located at the peripheral edge of the recess 6, facing the inner upper wall 7. The inner upper wall 7 intersects the inner side wall 2 by defining an intersection zone 8 in the shape of a circle. As illustrated in FIG. 3, the surface of the internal lateral wall 2 is configured so that a straight line D passing through the focus 1 10 of the collimator 200 and the intersection 8 between the inner upper wall 7 and the internal lateral wall 2 is tangential to the inner side wall 2. For this purpose, the surface of the inner side wall 2 and the surface of the peripheral reflection wall 3 can be calculated in two separate ways. According to a first possibility, the internal lateral wall 2 is calculated to have a predefined geometry with symmetry of revolution around the optical axis 5, for example a circular arc or continuous curvilinear shape. Then the surface of the inner side wall 2 is calculated to have a tangent at the point of intersection 8 with the inner upper wall 7 passing through the focus 1. The other parameters of the inner side wall 2 are arbitrarily defined. Then, a bundle of light rays starting from the focus 1 and intercepting the inner side wall 2 are considered according to the law of refraction n1 x sin (II) = n2 x sin (i2). These light rays transmitted by the inner side wall 2 will intercept the peripheral reflection wall 3. The surface of the latter is then calculated using a photometric optimization software, such as LightTools, so that the After a second possibility, the surfaces of the inner side wall 2 and of the peripheral reflection wall 3 are simultaneously calculated with the objective that: - A bundle of light rays from the hearth 1 collimator spring 30 200 being parallel to the optical axis 5 "far-field optimization" - A bundle of light rays from the hearth 1 emerges from the collimator 200 being regularly ordered along the outlet wall 4 "Near field optimization". This construction technique makes it possible to leave free choice on two parameters: the tangent of the internal lateral wall 2 at the vertex, that is to say at the intersection 8 with the internal upper wall, and the tangent of the lateral wall internal 2 at the base, that is to say, at the intersection 9 with the peripheral reflection wall 3. It is then possible with this technique to fix that the tangent to the vertex passes through the focus 1 of the collimator 200.
    [0004] The construction of the tangent of the inner lateral wall 2 at the top also defines the starting point of the surface of the inner upper wall 7. The convex surface of the inner upper wall 7 is moreover conventionally configured, so as to transmit everything the rays from the focus 1 into a collimated beam.
    [0005] Furthermore, according to a possibility not shown, the outlet wall 4 is shared between a central zone whose periphery has the shape of a circle and a peripheral zone encircling the central zone. In case, the central zone is configured to operate in association with the inner upper wall 7 and the peripheral zone is configured to operate in association with the inner side wall 2. This configuration is obtained in particular by generalizing the principles of calculation mentioned above including these areas. The collimator 200 thus configured prevents Fresnel losses. The p-rays that would have led to the formation of the parasitic ring in a conventional configuration are reflected on the inner side wall 2 with a grazing angle of incidence so that these rays p are directed towards the inner upper wall 7 where they are collected as if they came directly from a point near the focus 1, as illustrated by the dashed lines defining a virtual radius. These reflected p-rays then add to the main beam so that the latter gains in light intensity while limiting the formation of a parasitic ring.
    [0006] FIG. 4 illustrates the path of a luminous ray e from the periphery of the light source and that of a luminous ray from the focus 1. This ray i from the focus 1 is transmitted to the point A of a convex portion 11 of the inner side wall 2, is reflected at the point A 'of the peripheral reflection wall 3 to emerge from the outlet wall 4 substantially coaxially with the optical axis 5.
    [0007] The radius e coming from the periphery of the source is transmitted to point B on the convex portion 11 of the inner side wall 2. The extension of this ray e forms a virtual ray which passes through A. Then this ray e is collected on wall peripheral reflection 3 at point B 'to be returned to the outlet wall 4 so as to emerge at a small angle with the optical axis 5. This ray e is then added to the collimated beam, unlike a radius e from the same point away from the focus 1 in a conventional collimator 100 as illustrated in FIG. 2.
    [0008] Thus, the configuration of the convex portion 11 makes it possible to intercept the incident rays far away from the focus 1 much earlier because of its lower position compared to a rectilinear side wall. The radius e is redirected towards the peripheral reflection wall 3 instead of forming parasitic light (FIG. 2) or leading to losses. The surface of this convex portion 11 is determined by considering a central radius from the focus 1 and refracted on the inner side wall 2 at any intercept point A and a marginal radius away from the focus 1 also passing virtually through the same point A The extension of the marginal beam, called virtual radius, is shown in dashed line. Physically the marginal radius intercepts the surface of the convex portion 11 at a point B distinct from the point A. A point A 'defines the point of reflection on the peripheral reflection wall 3 of the central ray and a point B' defined the point of reflection on the peripheral reflection wall 3 of the marginal radius. The surface of the inner lateral wall 2 and that of the peripheral reflection wall 3 are then calculated according to one of the methods explained above taking into account two additional constraints: the points A and B must be distinct and A ' must be farther away from home 1 than is B '. Figures 4, 6 and 7 each illustrate an embodiment which differs one from the other by the configuration of the tangent to the base of the inner side wall 2. It is inclined at an angle of about 20 ° with respect to the optical axis 5 in Figure 4, an angle close to 0 ° in Figure 6 and 0 ° in Figure 7. These different angles can achieve an optimized light intensity. Indeed, these configurations are chosen so that the inner side wall 2 comprises an annular zone 12 defined from the focus 1 at a solid angle α (alpha) ranging from 35 ° to 90 ° with respect to the optical axis 5 and so that the tangent of the annular zone 12 forms an angle 0 (beta) which can vary between 0 ° and 30 ° with respect to the optical axis 5 (refer to FIG. 5). This annular zone 12 then has a weakly pronounced slope with respect to the optical axis 5 so that its peripheral end is closer to the light source which then illuminates a large area in the vicinity of the surface 4. According to the law of conservation of the geometric extent, the light beam is all the more intense as its section is large. The annular zone 12 as defined thus makes it possible to improve the luminous intensity of the collimated beam.
    [0009] Moreover, the collimator 200 is monoblock. It is preferably made of a polymer, such as silicone, which gives flexibility to the collimator 200. This makes it easier to demold the collimator 200 despite the convex portion 11 of the inner side wall 2 which forms an undercut. . Thus, the present invention proposes a collimator 200 which makes it possible to limit the losses of Fresnel, to avoid the formation of a parasitic ring, to refocus the beams on the periphery of the light source, to increase the luminous intensity and to use large light sources. In addition, this collimator 200 formed of silicone is monobloc for a short manufacturing process and simple to achieve. It goes without saying that the invention is not limited to the embodiment described above by way of example but that it includes all the technical equivalents and variants of the means described as well as their combinations. 15
    权利要求:
    Claims (12)
    [0001]
    REVENDICATIONS1. Optical collimator (200) for collimating a beam from a light source, the collimator (200) having an overall shape of a bowl, the collimator (200) comprising a symmetry of revolution about an optical axis (5) of the collimator (200), an outlet wall (4), an inlet recess (6) opposite the outlet wall (4), the inlet recess (6) being defined by an inner side wall (2) and an inner upper wall (7) contiguous with the inner side wall (2) so as to define an intersection zone (8), the inner side wall (2) and the inner top wall (7) being intended for the peripheral and central input of a light beam incident in the collimator (200), a peripheral reflection wall (3) joining the outlet wall (4) to the inner side wall (2), the surface of the inner side wall (2) being configured so that a straight line (D) tangent to the side wall dull (2) and joining the intersection zone (8) passes through the focus (1) of the collimator (200).
    [0002]
    2. Optical collimator (200) according to claim 1, wherein the inner side wall (2) has a curvilinear surface with symmetry of revolution about the optical axis (5) of the collimator (200). 20
    [0003]
    3. Collimator (200) according to one of claims 1 to 2, wherein the inner side wall (2) comprises a convex portion (11) configured to intercept at one point (A) a radius (i) central from the focus (1) and a virtual marginal radius extending a real marginal radius (e) from the periphery of the light source, the actual marginal radius (e) being intercepted at a point (B) of the inner side wall (2), and so that the peripheral reflection wall (3) reflects the central radius (i) at a point (A ') and the actual marginal radius (e) at a point (B') with the point (A) ) distinct from the point (B) and the point (A ') having a distance from the focus (1) more important than the point (B').
    [0004]
    4. Collimator (200) according to one of claims 1 to 3, wherein the inner side wall (2) comprises an annular zone (12) defined from the focus (1) at a solid angle (a) between 35 ° and 90 ° with respect to the optical axis (5), and wherein the tangent of the annular zone (12) forms an angle ((3) between 0 ° and 30 ° with respect to the optical axis (5). ).
    [0005]
    5. Collimator (200) according to one of claims 1 to 4, wherein the collimator (200) is monobloc.
    [0006]
    6. Collimator (200) according to one of claims 1 to 5, the collimator (200) is made of polymer.
    [0007]
    The collimator (200) of claim 6, wherein the polymer is a silicone.
    [0008]
    8. Collimator (200) according to one of claims 1 to 7, wherein the inner upper wall (7) comprises a portion having a convex surface, so as to converge the light rays from the home (1).
    [0009]
    9. Collimator (200) according to one of claims 1 to 8, wherein the outlet wall (4) comprises a portion having a substantially flat surface.
    [0010]
    10. A collimator (200) according to one of claims 1 to 9, wherein the outlet wall (4) comprises a portion having a substantially concave surface.
    [0011]
    The collimator (200) according to one of claims 1 to 10, wherein the exit wall (4) is partitioned between a central area and a peripheral area, the area of the central area being configured to share the refraction. incident light rays with the inner top wall (7) and the surface of the peripheral area being configured to operate in association with the peripheral reflection wall (3).
    [0012]
    The collimator (200) according to one of claims 1 to 11, wherein the output wall (4) present comprises a microtexturation configured to generate a type of light beam from the light source, such as a beam intermediate, a wide beam or an elliptical beam.
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    同族专利:
    公开号 | 公开日
    EP3123076B1|2019-06-26|
    WO2015145026A1|2015-10-01|
    EP3123076A1|2017-02-01|
    FR3019314B1|2017-08-11|
    CA2943909A1|2015-10-01|
    US10101591B2|2018-10-16|
    US20170139223A1|2017-05-18|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
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    US20090268166A1|2008-04-29|2009-10-29|Himax Display, Inc.|Projection system|
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    RU2670177C2|2011-12-13|2018-10-18|Филипс Лайтинг Холдинг Б.В.|Optical collimator for led lights|US10543778B2|2017-09-25|2020-01-28|Ford Global Technologies, Llc|Light assembly for vehicle and method of using the same|
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    DE102018101291B4|2018-01-22|2020-10-29|Hans-Erich Gubela|Use and method for producing an elastic retroreflector|
    法律状态:
    2016-01-21| PLFP| Fee payment|Year of fee payment: 3 |
    2017-01-19| PLFP| Fee payment|Year of fee payment: 4 |
    2018-02-08| PLFP| Fee payment|Year of fee payment: 5 |
    2020-01-23| PLFP| Fee payment|Year of fee payment: 7 |
    2021-12-10| ST| Notification of lapse|Effective date: 20211105 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1452747A|FR3019314B1|2014-03-28|2014-03-28|LIGHT COLLIMATOR|FR1452747A| FR3019314B1|2014-03-28|2014-03-28|LIGHT COLLIMATOR|
    US15/300,100| US10101591B2|2014-03-28|2015-03-18|Optical collimator|
    PCT/FR2015/050655| WO2015145026A1|2014-03-28|2015-03-18|Optical collimator|
    EP15714875.0A| EP3123076B1|2014-03-28|2015-03-18|Optical collimator|
    CA2943909A| CA2943909A1|2014-03-28|2015-03-18|Optical collimator|
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