Abstract:
A headlight, in particular, for motor vehicles, has an elongated incandescent body ( 2 ) with an incandescent body longitudinal axis ( 4 ), a reflector, associated with the incandescent body ( 2 ) for bundling of the light emitted from the incandescent body ( 8 ), and a photoconductor ( 8 ), in which the light emitted from the reflector ( 6 ) in the direction of an optical axis is coupled-in by means of a coupling-in surface ( 12 ) of the photoconductor ( 8 ). The incandescent body longitudinal axis ( 4 ) forms an angle (α) with the optical axis ( 10 ) that is greater than 0 degrees.

Description:
BACKGROUND OF THE INVENTION 
   The present invention relates to a headlight, in particular, for a motor vehicle, with an elongated incandescent body with an incandescent body axis, with a reflector associated with the incandescent body for beaming or bundling of the light emitted from the incandescent body, as well as with a photoconductor, in which the emitted light from the reflector in the direction of an optical axis is coupled in by means of a coupling-in surface of the photoconductor. 
   This type of headlight is known from the prior art. Photoconductor elements are used more than other components, because they can be made with varying structures. The design freedom of elements for the outer illumination of motor vehicles includes an increasingly greater meaning for the appearance of a vehicle. An aesthetically pleasing design of the vehicle and the elements for the outer illumination makes possible the production of different features in contrast to competing motor vehicle productions on the market. 
   The use of photoconductor elements has the advantage that a spatial separation between the production of the light by means of a light source on the one hand and the radiation of the light in an outer region of the motor vehicle on the other hand can take place. In this connection, it is necessary that the light produced is conducted to a point via photoconductors of the respective elements, which, in particular, can be provided in the photoconductor itself and which radiates the light in an outer region of the motor vehicle. The photoconductors can be installed as desired in the motor vehicle and demand proportionally little space. For coupling-in of the light in the photoconductor, a light source is used for radiating the light that is bundled from a reflector and is coupled in an end cross section of the photoconductor. The end cross section of the photoconductor is subsequently designated as the “coupling-in surface”. The photoconductor conducts the light further, then relatively loss-free, to the so-called “uncoupling location”. 
   According to the state of the art, devices for a photoconducting coupling-in are known, in which an elongated incandescent body with an incandescent body longitudinal axis is directed axially parallel to an optical axis, along which the central longitudinal axis of a photoconductor with a circular cross section, at least in the area of the coupling-in surface, is arranged. That is, the optical axis cuts the coupling-in surface and does this preferably at a 90° angle. These types of devices have the disadvantage that the cross section of the photoconductor, or its coupling-in surface, must be relatively large and reflection of the light source is a little compressed. Thus, the brightness separation is produced on the coupling-in surface of the photo conducting elements, which is optimal only in partial regions. 
   The present invention addresses the underlying problem of making available a headlight, in particular, for motor vehicles, with which an advantageous brightness separation on the coupling-in surface of a photoconductor element is produced with the smallest possible cross section of the coupling-in surface. 
   SUMMARY OF THE INVENTION 
   The above-stated problem is resolved with a headlight according to the present invention, whose incandescent body&#39;s longitudinal axis forms an angle with the optical axis that is greater than 0°. 
   The incandescent body used in the headlight is elongated and has an incandescent body longitudinal axis. This incandescent body is associated with a reflector for bundling of the light radiated from the incandescent body. The emitted light is coupled-in in the direction of an optical axis in a coupling-in surface of a photoconductor. In this manner, the individual light beams do not run necessarily completely parallel to the optical axis. The light emission direction, however, can be described essentially through the optical axis. The optical axis corresponds, therefore, also to the longitudinal axis of the reflector. The central longitudinal axis of the photoconductor overlaps with the direction of the optical axis at least in the region of the coupling-in surface. In particular, however, the optical axis cuts the coupling-in surface, preferably at a 90° angle. The optical axis and the incandescent body longitudinal axis, then, do not form an angle of 0°, as with common systems, rather an angle deviating there from. Advantageously, the angle between the incandescent body and the optical axis is 90°; however, the angle also can be in a range of between 0 and 90°, that is, in a range of 0-30°, 30-45°, 45-60°, or 60-90°. It is important, that the incandescent body longitudinal axis and the optical axis from an angle with one another that is not 0°. In this manner, it is possible that the incandescent body images emitted from the incandescent body and bundled from the reflector can be more greatly compressed and the coupling-in surface of the photoconductor can be selected to be substantially smaller than with conventional photoconductor coupling-in devices. In particular, incandescent body images are achievable, which have a large or small projection surface. The arrangement of the incandescent body images and the frequency of the varying large and small projection surfaces make possible an adaptation of the coupling-in surface of the photoconductor, as well as the entire cross section of the photoconductor to the effect that a minimization is achieved, compared with common, axial photoconductor coupling-in devices. 
   The cross section of the photoconductor and/or its coupling-in surface can deviate from a circular shape and have a varying extension in the longitudinal and transverse direction. Approximately square or elliptical or rhombus shapes are contemplated, for example. The maximal extension of the photoconductor runs with an elliptical or rhombus shape of the photoconductor and/or its coupling-in surface in the direction of the longitudinal extension of the cross section. With an ellipse, this corresponds with the direction of the longitudinal radius and with a rhombus, with the direction of the longitudinal diagonal. In the case of a photoconductor and/or a coupling-in surface with an approximately square shape, the maximal extension of the cross section runs in a direction, which diverges from the direction of the longitudinal extension of the square cross section, namely, in the direction of one of the diagonals. The noted shapes represent advantageous examples; however, all cross sections of the photoconductor and/or coupling-in surface that depart from a circular shape are possible. 
   To achieve a homogenous brightness separation, it is advantageous that the photoconductor is arranged such that the incandescent body image with the large projection surface lies parallel to the maximum extension of the coupling-in surface. The images with the large projection surface extend in the direction of the maximal extension of the coupling-in surface, as well as parallel thereto. Therefore, the orientation of the incandescent body image with the large projection surface are not varied about 360°, as with common devices for photoconducting coupling with photo conductors having circular cross sections; rather, the orientation of the incandescent body image with the large projection surface is determined based on the maximum extension of the coupling-in surface. In order to achieve an advantageous brightness separation, it is also advantageous that the incandescent body image is coupled in with small projection surfaces in the region of the coupling-in surfaces, which are not covered, or only partially covered, by the incandescent body images with large projection surfaces. It can therefore be provided that the reflector is correspondingly designed. 
   For the proposed arrangement of the incandescent body, reflector, and photoconductor, or incandescent body longitudinal axis and optical axis, it is not important if the incandescent body, that is, the element which directly emits light, is held by an element that has a longitudinal axis that runs in the direction of the incandescent longitudinal axis or if the element supporting the incandescent body is arranged in the direction of the optical axis or in a desired intermediate position between the optical axis and the incandescent body longitudinal axis. It is only important that the light-emitting element, that is the incandescent body with its incandescent body longitudinal axis from an angle with the optical angle that is greater than 0°. The incandescent body, as well as the incandescent coils, is formed such that the use of conventional incandescent lamps is possible. It can also be structured, however, from an arc lamp, which, for example, is can be made from a gas discharge tube, or glow lamp. Other incandescent body designs are also contemplated, however, as long as these have a longitudinal extension. 
   Further advantageous forms and features of the invention are provided in the following description as well as the above disclosure, in which the invention is described and explained in detail with reference to the accompanying drawings. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  shows a sectional view of the headlight of the present invention; 
       FIG. 2  shows a sectional view of the headlight in the plane I—I from  FIG. 1 ; 
       FIG. 3  shows a plane view on a coupling-in surface; and 
       FIG. 4  shows an incandescent body image on coupling-in surfaces of two photoconductors. 
   

   DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
   In  FIG. 1 , an elongated incandescent body  2  with an incandescent body longitudinal axis  4  is illustrated, whereby the incandescent body is associated with a reflector  6 , which deflects light emitted from the incandescent body  2  in the direction of an optical axis  10  and which is coupled in a photoconductor  8 . The photoconductor  8  has a coupling-in surface  12 . The incandescent body longitudinal axis  4  and the optical axis  10  are disposed at an angle α=90° from one another. 
   The incandescent body  2  is arranged in a retainer element  14 , which in turn, is hold by a glass bulb. The glass bulb  16  is fixed in a socket  18 . 
   The incandescent body  2 , that is, the light-producing element, has an arc-shaped structure and is, for example, produced by means of a gas discharge. A light beam  20  emitted from this incandescent body  2  impinges in a reflection point  22  of the inner side  24  of the reflector  6  and is there diverted in the direction  20 ′ on the coupling-in surface  12 . A light beam  26  is likewise diverted in the reflection point  22  in the direction  26 ′ and impinges in a coupling-in point  28  on the coupling-in surface  12 . The light beams  30  and  32 , which are emitted from the incandescent body  2 , are diverted in the direction  30 ′ or  32 ′ from the reflector inner side  24  and impinge in the coupling-in point  25  and in a coupling-in point  34  on the coupling-in surface  12  of the photoconductor  8 . The coinciding of the light beams  20 ′ and  32 ′ in a coupling-in point  25  can be determined by means of the structure of the reflector. However, also disintegration is possible and is achievable by means of a determined reflector construction. 
   The distance  36  between the coupling-in point  25  and  28  of the diverted light beams  20 ′ and  26 ′ is recognizably larger than the distance  38  between the coupling-in points  25  and  34  of the diverted light beams  30 ′ and  32 ′. Thus, incandescent body images are projected on the coupling-in surface  12  of the photoconductor  8 , whose extension is variably large. 
     FIG. 2  shows a sectional view of the headlight in the plane I—I in FIG.  1 . The light beams emitted from the incandescent body  2  are projected from the inner side  24  of the reflector  6  onto the coupling-in surface  12  of the photoconductor. For example, the light beams  40  and  42  are diverted in the direction  40 ′ and  42 ′ and impinge in the coupling-points  44  and  46  on the coupling-in surface  12  of the photoconductor  8 . In addition, the light beams  48  and  50  are diverted in the direction  48 ′ and  50 ′ and impinge in the coupling-in point  44  and in a coupling-in point  52  on the coupling-in surface  12 . Also here, by means of the structures of the reflector and the positioning of the optical axis  10  to the incandescent axis  4 , various sizes of incandescent body images are produced. 
     FIG. 3  shows a top plan view on the coupling-in surface  12 , which is limited by a periphery  54  and has a longitudinal extension  56  as well as a transverse extension  58 . The maximum extension of the cross section of the coupling-in surface  12  lies in the diagonal  60  of the diagonal direction  62 . On the coupling-in surface  12 , for example, individual incandescent body images are represented, from which, in turn, for example, an incandescent body image with a large projection surface  64  and an incandescent body image with a small projection surface are emphasized. The incandescent body image  64  extends essentially in the direction of the maximum extension  60  of the coupling-in surface  12 . The incandescent body image  66  with the small projection surface lies in a region of the coupling-in surface  12 , which is not covered or only partially covered by the incandescent body image  64  with the large projection surface. 
   With overlapping of the incandescent body images emphasized by way of example in  FIG. 3  with large and small projection surfaces, it is clear that a brightness separation is achievable, in which the light separation is better utilized. 
     FIG. 4  shows two illustrated coupling-in surfaces lying over one another with peripheries  68  and  70 . The periphery  60  is determined from an essentially circularly shaped photoconductor cross section, as used in headlights with conventional photoconductor coupling-in devices, that is, with which the optical coincides with the incandescent body longitudinal axis. The periphery  70  shows an inventive minimized embodiment of a photoconductor cross section with a longitudinal extension  72  and a transverse extension  74 . 
   With use of conventional photoconductor coupling-in devices, incandescent body images are projected on a coupling-in surface with an essentially circular cross section. In  FIG. 4 , for example, individual coupling-in images  76  are shows. By overlapping of these coupling-in images, an impression can be introduced, in which brightness separation in the coupling-in surface of the photoconductor cross section is achievable. It is to be recognized from  FIG. 4  that a homogenous and the brightness separation well-utilized by the photoconductor is only ensured in a central region of the photoconductor cross section  68 . However, with an inventive arrangement and by using a photoconductor with the cross section  70 , which is smaller, by overlapping of incandescent images  78  shown by way of example, a brightness separation is produced, which qualitatively at least corresponds to the brightness separation on the circular cross section  68  upon use of conventional photoconductor coupling-in devices. The spaced required by the photoconductor  70 , however, is substantially smaller than the cross section of photoconductors with circular cross sections.