1. Field of the Invention
The invention concerns a lighting or signaling device for a motor vehicle which comprises a plate for guiding the light.
The invention more particularly concerns a lighting or signaling device for a motor vehicle which is capable of emitting a linear beam essentially in the direction of an optical axis, and which comprises:
a point light source that emits light rays radially around a source axis; and
a light ray guiding plate that comprises an edge for inputting the light rays, a front edge for outputting the light rays tangentially to the light guiding plate, and a rear edge for reflecting the light rays coming from the light source in the direction of the output edge.
2. Description of the Related Art
It is common practice to group several lighting and/or signaling functions together in a single enclosure, so as to simplify the electrical wiring for these different functions in a motor vehicle.
Moreover, the shape of the lighting and/or signaling lights plays a leading role in the search for a style and original aesthetics which will enable the motor vehicle to be recognized from a distance.
To solve these problems, equipping the vehicle with light guides is known. A light guide is a cylinder of transparent material which forms a kind of “pipe” into which the light rays enter via a first input end. The light rays are then guided along the light guide by successive total reflections on its cylindrical outer face.
A rear portion of the cylindrical face of the light guide comprises irregularities, such as diffusion flutes, which make it possible to diffuse some of the light rays towards the front so that some of the diffused light rays exit the light guide by passing through the opposite portion of the cylindrical face in order to form a light beam.
The light guide can for example be shaped as a ring that surrounds the front boundary of a low beam headlamp so as to emit an annular light beam. The input end portion of the light guide is then bent so that the light ray input end is arranged outside the ring formed by the light guide.
However, such a solution does not make it possible to obtain a high intensity light beam. This is because the light rays emitted by the light source are guided in a random and unordered manner inside the light guide. Moreover, only some of the light rays are diffused to the outside by the irregularities. Consequently, the light beam obtained by such a device is very weak even if the light source arranged at the input end of the light guide is very powerful.
However, certain lighting and signaling functions require a very intense light beam in order to comply with current regulations. The light guide is therefore not suitable for implementing such functions.
Moreover, the appearance of the annular beam obtained is highly non-uniform in particular for the following two reasons.
On the one hand the material constituting the lighting or signaling device brings about some absorption of the light rays that pass through it, which results in losses that become greater with the distance away from the light source. As a result the brightness in the vicinity of the light source is greater than at a distance from this source, hence a uniformity fault.
On the other hand some of the light rays introduced into the light guide via the bent input portion directly reach the opposite face of the light guide thus causing the appearance of a spot that is very bright compared with the rest of the annular beam.
There is, therefore, a need to provide an improved lighting or signaling device.
To solve these problems, the invention proposes a lighting or signaling device for a motor vehicle comprising a light source and a light ray guiding plate which comprises an edge for inputting the light rays, a front edge for outputting the light rays tangentially to the light guiding plate, and a rear edge for reflecting the light rays coming from the light source in the direction of the output edge, in which:
the light guiding plate comprises an area for coupling with the light source shaped so that the light rays emitted by the light source are propagated radially at the coupling area around a source axis;
the light guiding plate is shaped so that the light rays propagate in meridian incident propagation planes normal to the plate between the light source and the reflection edge, and in reflected propagation planes normal to the plate between the reflection edge and the output edge; and
the reflection edge is shaped so that the reflected propagation planes have an orientation with respect to the optical axis such that the lighting device is capable of emitting a linear light beam along an essentially longitudinal optical axis.
According to other characteristics of the invention:
the reflected propagation planes are parallel to the optical axis of the lighting device;
the reflected propagation planes are orthogonal to the output edge;
the light guiding plate (12) has a curved shape;
at least a first rear portion of the light guiding plate which is delimited by an angular sector extending from the source axis and which surrounds the reflection edge, has the shape of a portion of base sphere;
the source axis passes through the center of the base sphere;
a second front portion of the light guiding plate forms a solid of revolution around the optical axis that passes through the center of the base sphere;
the reflected propagation planes are secants along the optical axis;
at least two light guiding plates are arranged in a first stratum, at least a third light guiding plate being arranged in a second stratum, each light guiding plate being a portion of a base sphere;
the light guiding plates of the first stratum are portions of a first common base sphere, and in that the light guiding plates of the second stratum are portions of a second common base sphere, all the light guiding plates being centered on a common center;
the light guiding plates have different axes and different radii of curvature;
the light ray output edge comprises means for defining the spread of the light beam around the direction of the optical axis in the reflected propagation plane;
the output edge is shaped like a lens in order to deviate the light rays by refraction;
the light guiding plate is flat;
the output edge forms an angle with the normal to the optical axis at several of its points and is capable of refracting the outgoing light rays, the reflection edge being shaped so that the reflected propagation planes have an orientation with respect to the output edge such that the light rays are essentially parallel or parallel to the optical axis once refracted by the output edge; in the absence of flutes on the output edge, the light rays refracted by the output edge will be parallel to the optical axis; in the presence of flutes spreading the light horizontally, the light rays refracted by the output edge will be essentially parallel to the optical axis, and the beam exiting each flute will be centered on an axis parallel to the optical axis;
the output edge is essentially flat, the reflection edge having at least one parabolic shape whereof the directrix forms an angle with the normal to the output edge such that the light rays are essentially parallel or parallel to the optical axis once refracted by the output edge; in the absence of flutes on the output edge, the light rays refracted by the output edge will be parallel to the optical axis; in the presence of flutes spreading the light horizontally, the light rays refracted by the output edge will be essentially parallel to the optical axis, and the beam exiting each flute will be centered on an axis parallel to the optical axis;
the output edge is curved, the reflection edge having a complex shape such that, for any point on the output edge, any ray reflected by the reflection edge arriving at this point on the output edge is refracted parallel to the optical axis;
the output edge comprises means for defining the spread of the light beam in a plane tangential to the light guiding plate;
the output edge comprises flutes that are capable of deviating the outgoing light rays by refraction in a plane tangential to the light guiding plate;
the light guiding plate comprises holes that are arranged in proximity to the output edge, the light rays being deviated from their path in a tangential plane by passing through the wall of the hole before entering the light guiding plate again in the direction of the output edge;
the holes are aligned in staggered rows parallel to the output edge;
the light ray input edge comprises a front portion that is shaped so as to disperse the light rays coming from the light source heading directly towards the output edge;
the light source is a radially emitting LED and the light guiding plate comprises an aperture having a peripheral edge that corresponds to the input edge, the radially emitting LED being placed inside the aperture;
the light source is an axially emitting LED and the light guiding plate comprises a reflection surface corresponding to a shape complementary to a cone whereof the axis of symmetry corresponds to the source axis of the light source, this reflection surface being arranged opposite the input edge in order to direct the light rays radially in the light guiding plate;
preferentially the complementary shape comprises a part with a conical profile and a flat part, the part with the conical profile being surrounded by the reflection edge and the flat part being oriented facing the output edge so that the rays emitted at the flat part are reflected parallel to a preferred direction, for example the optical axis; thus, all the rays arriving on the shape with the conical profile are reflected towards the reflection edge, whereas those which would not be able to reach this reflection edge if the complementary shape had a completely conical profile, reach the flat surface and are therefore reflected parallel; the optical efficiency of the device is thus increased;
the light source is arranged at a distance from the input edge, the emitted light rays being guided as far as the reflection face in the shape of an angular sector of a cone with source axis in order to direct the light rays radially solely towards the reflection edge of the light guiding plate.
Other characteristics and advantages will emerge from a reading of the following detailed description, for the understanding of which reference should be made to the accompanying drawings, amongst which:
Subsequently, identical, analogous or similar elements will be designated by the same reference numbers.
For the remainder of the description, there will be adopted on a non-limiting basis a longitudinal orientation fixed with respect to the motor vehicle and directed from the rear to the front which is indicated by the arrow “L” in
The lighting device 10 comprises in particular at least one light guiding plate 12 which appears in the form of a portion of a segment of a sphere. The lighting device 10 depicted in
For the remainder of the description, there will be adopted locally at any point of the light guiding plate 12, and on a non-limiting basis, a normal orientation N orthogonal to the light guiding plate.
The light guiding plate 12 is thus delimited in the thickness direction by a front face 14 and a rear face 16 for guiding the light. The two faces, front 14 and rear 16, are parallel to each other over at least part of the plate.
The light guiding plate 12 is in particular delimited laterally by a front edge 18 for outputting the light rays and by a rear edge 20 for reflecting the light. In the example depicted in
The reflection edge 20 can consist of a reflective plate, such as an aluminized coating on the outer face of the reflection edge 20. It can also be provided that, between the two junctions between the reflection edge 20 and each of the faces 14 and 16 of the light guiding plate 12, the output edge 18 has a ridge extending along this edge and dividing it into two faces forming an angle between them. Thus an incident ray RI (
The boundary of the light output edge 18 here forms a flat arc of a circle, that is to say the boundary of the output edge is defined by the intersection between the base sphere 13 and a plane.
According to a variant of the invention depicted in
As depicted in
The light source 28 is capable of emitting light rays in an essentially radial direction around a source axis “S” that is normal to the light guiding plate 12. More precisely, the light source 28 is capable of emitting a fan of light rays radially at least towards the rear in the direction of the reflection edge 20.
The light source 28 is here a so-called “Side Emitter” light emitting diode or “LED” which emits light rays in a fan for example of approximately 30° either side of the radial direction in a plane meridian to the source axis “S” and which is capable of extending around the source axis “S”, for example over 360° in a plane normal to the source axis “S”.
As depicted in
According to variants depicted in
According to the variant depicted in
The cone “CO” can also have a deformed area making it possible to send back the rays that, without this area, would directly reach the output edge. This concerns for example a kind of “truncation” so that the reflection area “CO” has a flat face. Thus, according to a section along a plane perpendicular to the source axis “S” and approximately at the face of the light guiding plate which is opposite the LED 28, the perimeter of the cone corresponds to a circle. With the truncation, a section is obtained in the form of a circle in which an arc of a circle has been removed, a straight line connecting the two ends of the remaining part of the circle. A flattened circle is therefore obtained. This straight line constitutes the base of the triangle formed by the truncation on the cone. The tip of this triangle opposite to this base is situated on the cone between the two faces of the light guiding plate, preferentially in proximity to the tip of the cone. A cone with a flatted face is therefore obtained. This flattened face is situated facing the output edge. All the rays emitted above the part with the conical profile will therefore be distributed around the source axis “S” inside an angular interval corresponding to the circular part of the section of the cone on the face opposite to the LED 28. Preferentially the tip of the flat face is situated between the tip of the cone and the base thereof, on the side of the output edge (for example on the left in
In conclusion on the choice of LEDs, it can be seen that one embodiment of the invention makes it possible to use LEDs with very different characteristics, capable of emitting either radially, or axially, or in a half-plane. It is then necessary to arrange the coupling area accordingly, for example by making an opening that is either through or not for inserting therein all or part of the LED, and by providing optical means when necessary (in particular for LEDs emitting in a half-plane) so that the maximum amount of the light emitted by the LED propagates correctly in the thickness of the coupling area without loss as far as the rear reflection area 20.
In the examples depicted, the light input edge 26 is thus surrounded by the external boundary comprising the output edge 18 and by the reflection edge 20 of the light guiding plate 12. The input edge 26 could however not be closed. This is because there is a sector of this edge 26 that is not very effective, situated opposite the reflection edge 20, and for which the rays reflected by the edge 20 return towards the input edge 26. These light rays are therefore not used in the lighting or signaling device, and they are lost. Advantage can be taken of this observation to not dispose any material in this region, in order to thus facilitate the removal of the light guiding plate from the mould.
The light guiding plate 12 is made from a transparent material whereof the refractive index is higher than the refractive index of the medium in which the lighting device 10 is intended to be immersed, air for example. Thus, a light ray introduced into the thickness of the plate 12 via its input edge 26 with an incident angle with respect to the normal “N” which is greater than a critical angle of refraction is capable of being totally reflected by the guidance faces 14, 16.
The light ray is therefore guided in the thickness of the light guiding plate by successive reflections between the two guidance faces 14, 16.
As depicted in
For the remainder of the description, an incident light ray will be defined as a light ray that is emitted by the light source 28 in the direction of the reflection edge 20. The light rays emitted by the light source 28 directly in the direction of the output edge 18 are therefore not included in this definition of incident rays. The light rays that are emitted towards the front by the light source 28 directly in the direction of the output edge 18 will be referred to as “direct”.
The light source 28 can also consist of an incandescent bulb, for example a halogen bulb, with axial filament, inserted within the boundary delimited by the input edge 26. Provision can then advantageously be made in this case that an area of the light guiding plate, in the vicinity of the input edge 26, is made of glass, while the remainder of the plate will be made of plastic overmolded on this glass area. Such a design makes it possible to avoid thermal problems that could be generated by the use of an incandescent source.
To avoid the input edge 26 being visible by an observer situated in the axis A, or more exactly to avoid this observer seeing a light spot, corresponding to the light source, surrounded by two black points, corresponding to the upper and lower faces of the input edge 26, it is advantageous to see to it that each point on the portion of the input edge 26 corresponding to the direct rays re-emits light towards a given area of the output edge.
For example a complex shape 29 can be given to the input edge 26, so that the light rays are collimated in the plane tangential to the plate, in order that these light rays reach a reduced area of the output edge 18. The addition of flutes on this complex shape 29 then makes it possible to optimize the concentration of the rays reaching the area of the output edge 18, and consequently also the size of this area of the output edge 18, in order that this area does not appear brighter than the rest of the boundary for an observer situated in the axis.
The portion of input edge 26 which is oriented towards the front is thus shaped so as to distribute the direct light rays substantially uniformly along the output edge 18. As depicted in
So that the direct light rays are collimated in the plane tangential to the plate, it is also possible to place on the area of the input edge corresponding to the direct rays, in front of the LED with respect to the optical axis, an area with the shape of a convex curved surface, facing the LED 28, the surface being curved in the direction of the LED. For example, the curved area can be put in place of the serrated area 29 depicted in
Similarly, provision can be made that the input edge 26 is in the shape of a slightly truncated cone, so as to optimize the mean direction of the rays in the plate in the meridian plane with respect to the tangent to the plate.
According to a variant depicted in
The light source 28 is for example a halogen bulb or a light emitting diode.
In the example depicted in
Advantageously, the reflection face 30 is shaped as a rear portion of cone so as to produce no “direct” light rays but only “incident” light rays.
Advantageously, the reflection face 30 forms an upper end face of the light guide 32 and the light guide 32 is made in one piece of material with the light guiding plate 12.
According to the teachings of the invention, the light guiding plate 12 is designed so that the incident light rays emitted towards the rear by the light source 28 propagate in the light guiding plate 12 along so-called “incident” meridian propagation planes “Mi” that radiate radially from the source axis “S”. Thus, each light ray is guided so as to follow a radial direction inside the light guiding plate 12 as far as the reflection edge 20. In
Moreover, the light guiding plate 12 is also designed so that the rays reflected by the reflection edge 20 propagate towards the front along so-called “reflected” flat propagation planes that are normal to the light guiding plate 12 between the reflection edge 20 and the output edge 18. The reflection edge 20 is more particularly shaped so that the reflected propagation planes “Mr” are oriented parallel to the optical axis “A”.
Thus, the reflected light rays are distributed parallel all along the output edge 18 so that each point of the output edge emits a substantially equal amount of light in the direction of the optical axis A. In this way, the output edge is seen uniformly by an observer looking at the output boundary in the axis A.
Advantageously, but non-limitatively, the reflected propagation planes “Mr” are orthogonal to the output edge 18 so that all the reflected light rays that reach the output edge 18 exit without loss of light intensity.
The reflection edge 20 is here perpendicular to the guidance faces 14, 16 of the light guiding plate 12.
This design is made possible on the one hand by the base sphere portion shape 13 of at least one rear portion 12R of the light guiding plate which is passed through by the incident light rays between the light source 28 and the reflection edge 20, and on the other hand by the particular shape given to the boundary of the reflection edge 20.
The rear portion 12R forms at least one angular sector extending from the source axis “S” and which surrounds the reflection edge 20.
On account of the rounded shape as a portion of base sphere 13 of the rear portion 12R of the light guiding plate 12, the reflected propagation planes “Mr” are secants along the same axis which passes through the center “O” of the base sphere and which is coincident with the optical axis “A”. Moreover, the source axis “S” is a secant with the optical axis “A” at the center “O” of the base sphere.
Furthermore, the boundary of the reflection edge 20 is defined mathematically by the following equation:
{right arrow over (dOM)}^({right arrow over (ui)}−{right arrow over (ur)})={right arrow over (0)}
“O” being the center of the base sphere of the rear portion of the light guiding plate 12;
“M” being any point on the reflection edge 20;
{right arrow over (dOM)} being the differential of the vector OM, that is to say the tangent at M to the boundary of the reflection edge 20;
{right arrow over (ui)} being a unit vector orthogonal to the incident meridian plane “Mi” passing through the point “M”;
{right arrow over (ur)} being a unit vector orthogonal to the reflected propagation plane “Mr” passing through the point “M”.
This equation expresses the fact that the image of an incident propagation plane “Mi” by the reflection edge 20 is a propagation plane “Mr”.
This differential equation is capable of being solved either by analytical means or numerically using a computer.
When the radius of the base sphere 13 tends to infinity, the light guiding plate 12 can be considered as flat. The reflection edge 20 then has the shape of a parabola and the reflected propagation planes “Mr” are parallel to one another.
However, when the radius of the base sphere 13 is finite, the shape of the reflection edge cannot be likened to a parabola.
The light guiding plates 12 depicted in the figures are here portions of segments of a sphere.
According to a non-depicted variant of the invention, the light guiding plate 12 has a more complex shape. To comply with the conditions described previously, it is however essential that a rear portion 12R of the light guiding plate 12 forms a portion of the base sphere.
On the other hand, whilst complying with the condition according to which the reflected propagation planes “Mr” are secants along the optical axis “A” and orthogonal to the light guiding plate 12, the other front portion 12F of the light guiding plate 12 which is passed through solely by the reflected rays can have various shapes. To do this, the guidance faces 14, 16 form surfaces of revolution around the optical axis “A” passing through the center “O” of the base sphere 13.
The radii of curvature of the cross-section of the light guiding plate 12 along the reflected propagation plane “Mr” are advantageously sufficiently large to avoid the incident light rays reaching one of the guidance faces 14, 16 with an angle greater than the critical angle of refraction and exiting the light guiding plate 12 before reaching the output edge 18.
For example, the light guiding plate 12 can have a front portion of flared shape.
According to another aspect of the invention, depending on the characteristics of the light beam “F” it is sought to obtain, the light guiding plate 12 is supplemented by known optical systems for focusing or on the contrary spreading the light rays forming the light beam “F” in a meridian plane and/or in a plane tangential to the light guiding plate 12.
To that end, the output edge 18 of the light guiding plate is here shaped as a linear lens.
The output edge 18 is for example inclined with respect to a direction normal to the plate 12 as depicted in
According to a variant depicted in
As depicted in
According to a variant of the invention which is depicted in
According to another aspect of the invention, as depicted in
The boundary of the output edge 18 is then defined as the intersection between the base sphere and a plane perpendicular to the optical axis “A”.
According to a variant of the invention depicted in
According to a non-depicted variant of the invention, it is also possible to obtain a light beam “F” of non-circular shape by means of light guiding plates whereof the output edge 18 is not in the shape of a flat arc of a circle. Thus, the boundary of the output edges 18 is obtained by the intersection between a base sphere and any surface whatsoever.
It is for example possible to arrange several light guiding plates which have different axes and different radii or curvature, for example for producing any boundary whatsoever consisting of several arcs of circles.
For example, in order to obtain a light beam “F” forming an elliptical ring, the boundary of the output edges 18 is obtained by the intersection between the base sphere 13 and a cylindrical surface of revolution. The output edges 18 then have a skewed boundary, that is to say one that is not flat. The light rays must therefore be redirected, for example by flutes 34, at their exit from the light guiding plate 12 in order to be directed in the essential direction of the optical axis “A”.
By virtue of the lighting or signaling device 10 according to the invention, the light rays coming from the light source 28 reach the output edge 18 without losing their intensity. This design therefore makes it possible to obtain a light beam “F” of linear shape, here in the shape of an arc of a circle.
Such a lighting or signaling device 10 has good efficiency, that is to say the intensity of the emitted light beam “F” is scarcely less strong than the intensity of the light source 28. For example, the light beam “F” can have an intensity of 600 Cd for a light source with a luminous flux of 25 Lm.
In general terms, it should be understood that the rear portion 12R of the light guiding plate 12 is advantageously a portion of base sphere in order to optimize the intensity of the light beam as much as possible.
However, the invention is also applicable to light guiding plates that have a shape of a portion of base ellipsoid that differs little from a base sphere so that the light rays deviate slightly from the propagation planes “Mr” and/or “Mi” without the intensity of the light beam being substantially degraded. This is the case in particular for ellipsoids whereof the diameters have relatively close dimensions.
The invention also concerns flat plates, such as for example that depicted in
According to
Three parabolas have been depicted but this is not limiting. In fact fewer or more can be provided. By using more parabolas and limiting them on the side, the distance from the focus of the parabola to the output edge is reduced, thus allowing the use of shallower light guiding plates.
According to a non-depicted variant embodiment, the output edge can have a non-straight shape, for example rounded. Under these conditions the shape of the reflection edge will have a complex shape, that is to say a shape distinct from a parabola, ellipse or other simple geometric shapes. For each portion of the output edge, positioning and orientation of the reflection edge are determined, such that the angle of the reflected ray “RR” is refracted as an outgoing ray “RS” parallel to the optical axis “A”.
It is possible to place flutes on the output edge, irrespective of the boundary of the output curve. These are flutes or holes 36 as defined previously, in order to make the distribution of the light intensity uniform over the output edge. Moreover, the rays exiting each flute will be distributed laterally but centered around the optical axis A.
According to another variant embodiment, the output edge is perpendicular to the optical axis, the reflection edge forming at least one parabola in the plane of the light guiding plate and whereof the directrix is parallel to this optical axis. The reflected rays are then contained in reflected propagation planes parallel to the optical axis. The output edge is preferentially provided with flutes or holes 36 as defined previously, in order to make the distribution of the light intensity uniform over the output edge. The rays exiting each flute will be distributed laterally but centered around the optical axis A.
While the form of apparatus herein described constitutes a preferred embodiment of this invention, it is to be understood that the invention is not limited to this precise form of apparatus, and that changes may be made therein without departing from the scope of the invention which is defined in the appended claims.
Number | Date | Country | Kind |
---|---|---|---|
06 06718 | Jul 2006 | FR | national |
This application is a continuation of U.S. Ser. No. 12/794,998 filed Jun. 7, 2010, which is a continuation of U.S. Ser. No. 11/780,672 filed Jul. 20, 2007, now issued as U.S. Pat. No. 7,731,400, which are incorporated herein by reference and made a part hereof. This application also claims priority to French Application No. 0606718 filed Jul. 21, 2006, which application is incorporated herein by reference and made a part hereof.
Number | Name | Date | Kind |
---|---|---|---|
6193383 | Onikiri et al. | Feb 2001 | B1 |
6247826 | Funamoto et al. | Jun 2001 | B1 |
6447155 | Kondo | Sep 2002 | B2 |
6536921 | Simon | Mar 2003 | B1 |
6598998 | West et al. | Jul 2003 | B2 |
6836611 | Popovic | Dec 2004 | B2 |
6871988 | Gebauer et al. | Mar 2005 | B2 |
6880945 | Knaack | Apr 2005 | B2 |
7021805 | Amano et al. | Apr 2006 | B2 |
7025482 | Yamashita | Apr 2006 | B2 |
7334932 | Klettke | Feb 2008 | B2 |
7503666 | Tamura | Mar 2009 | B2 |
7513670 | Yang et al. | Apr 2009 | B2 |
7585083 | Kim et al. | Sep 2009 | B2 |
7909496 | Matheson et al. | Mar 2011 | B2 |
7942560 | Holder et al. | May 2011 | B2 |
20010015899 | Kondo | Aug 2001 | A1 |
20060291244 | Yang et al. | Dec 2006 | A1 |
Number | Date | Country |
---|---|---|
19925363 | Dec 2000 | DE |
1126209 | Aug 2001 | EP |
2813654 | Mar 2002 | FR |
Number | Date | Country | |
---|---|---|---|
20120075876 A1 | Mar 2012 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 12794998 | Jun 2010 | US |
Child | 13310845 | US | |
Parent | 11780672 | Jul 2007 | US |
Child | 12794998 | US |