Abstract:
A light guide for interfacing between a light source having a light emitting surface with a first shape and a light receiver with a light receiving surface of a second shape. The light guide has a light emitting end having a first shape of substantially the same size as the first shape of the light emitting surface. A light receiving end has a second shape of substantially the same size as the second shape of the light receiving surface. A free form body between the light emitting end and the light receiving end causes a transition between the first and second shape.

Description:
RELATED APPLICATIONS 
     This application claims priority to U.S. Provisional Application No. 61/313,477 filed Mar. 12, 2010, which is hereby incorporated by reference in their entirety. 
    
    
     FIELD OF TECHNOLOGY 
     The present invention relates to fiber optics, and more specifically to a light guide between differently shaped light source and light receivers. 
     BACKGROUND 
     Fiber-optic light sources are generally well known and are used in a broad range of applications. For example, in the medical field, fiber-optic illuminators such as various light sources, fiber-optics, and endoscopes are widely used in endoscopy. Bulb-based medical fiber sources are currently manufactured by Stryker, Smith-Nephew, Storz, Olympus, and others. Light sources and fiber-optics are commonly used for microscopy illumination, with lamp-based products offered by Zeiss, Welch-Allyn, Dolan-Jenner, and others. Fiber-optic illumination systems are also used with industrial boroscopes and machine vision systems. While the preceding devices primarily provide ‘white’ light for illumination, other fiber-optic light sources providing ‘blue’ light in the wavelength range 420-490 nm are used in photodynamic therapy for pediatric hyperbilirubinemia. 
     Systems having light sources and fiber-optics for light transmission can also provide one or more defined wavelengths of light for fluorescent excitation in biological and other research fields. For many applications, a round beam spot is desired, for example, an exam light, a spot light and a fiber optic light. In the case of a fiber optic light, the goal is to deliver more light through a fiber bundle. A fiber bundle is comprised of numerous fiber strands tightly packed together. All the fiber strands end at a cylindrical metal ferell. The fiber strands are then bound and polished. Light comes in from one end of the fiber bundle and is emitted out from the other end of the fiber bundle. When the fiber bundle end is round, the effective light transmission area is round. If the incoming light beam is from a rectangular or square shaped light source, depending on the size, only portion of the light is transmitted or portion of the fiber strands are utilized resulting in inefficiency. 
     For example, the emitting area inside an LED package is the footprint of the die or die cluster, which usually has a square or rectangular shape. When a lens system is used to collect light from LED(s), the output beam is the image of the LED die and is thus square or rectangular. This square or rectangular output beam therefore does not match the round fiber end and causes inefficiency because some light is lost in the transition. For many applications, it is desirable that the output light in a range of wavelength or color different than the source. Some manufacturers use additional filters to achieve that, increasing system complexity and cost. With the inventive light guide, filters can be integrated with the light guide by film deposition or color doping. The output beams currently use devices such as LEDs that are closely tied to the fiber optics. However, the shape of the LEDs still results in some inefficiencies. Another light guide is a thin plate for a surface light source that generates a highly uniform light. Such a light guide still creates inefficiencies as light is lost between the light source and the light guide. 
     SUMMARY 
     One disclosed example relates to a light guide for interfacing between a light source having a light emitting surface with a first shape and a light receiver with a light receiving surface of a second shape. The light guide has a light emitting end having a first shape of substantially the same size as the first shape of the light emitting surface. A light receiving end has a second shape of substantially the same size as the second shape of the light receiving surface. A free form body between the light emitting end and the light receiving end causes a transition between the first and second shape. 
     Another example is a method of producing a light guide to interface a light source having a light emitting surface having a first shape with a light receiver having a light receiving surface of a second shape. A light emitting end of the light guide having a first shape of substantially the same size as the first shape of the light emitting surface is formed. A light receiving end having a second shape of substantially the same size as the second shape of the light receiving surface is formed. A free form body connecting the light emitting end and the light receiving end having a shape transitioning between the first and second shape is formed. 
     Additional aspects will be apparent to those of ordinary skill in the art in view of the detailed description of various embodiments, which is made with reference to the drawings, a brief description of which is provided below. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1A  is a perspective diagram of an example fiber optic interface involving a different shaped light source and receiver; 
         FIG. 1B  is a perspective diagram of an example fiber optic interface involving a different shaped source and receiver; 
         FIG. 2  is a side view of a light guide that allows efficient light transmission between different shaped light source and receiver surfaces in  FIGS. 1A-1B ; 
         FIG. 3  is a perspective view of the light guide in  FIG. 2 ; 
         FIGS. 4A-4D  are dimensional views of the various cross sections of the light guide in  FIG. 2 ; and 
         FIG. 5  is a front view of an alternative polygonal shaped end of a light guide. 
     
    
    
     While these examples are susceptible of embodiment in many different forms, there is shown in the drawings and will herein be described in detail preferred examples with the understanding that the present disclosure is to be considered as an exemplification and is not intended to limit the broad aspect to the embodiments illustrated. 
     DETAILED DESCRIPTION 
       FIG. 1A  shows an example prior art fiber optic system  100  including an incoming light source  102  that includes a rectangular shaped light emitting surface  104 . The rectangular shaped surface  104  may be a result of an LED package that is typically fabricated in a square or rectangular shape. The light is emitted from the light emitting surface  104  to a fiber bundle  106  via an interface surface  108  that is in a circular shape. Since the interface surface  108  at the end of the fiber bundle  106  is circular, the effective light transmission area is circular. If the incoming light beam is from a rectangular or square such as the light emitting surface  104 , depending on the size, only portion of the light is transmitted or portion of the fiber strands are utilized resulting in inefficiency in light transmission. The grid sections of the light emitting surface  104  in  FIG. 1A  represent the portion of light that is not transmitted to the fiber bundle  106 . 
       FIG. 1B  shows another example prior art fiber optic system  150  that suffers from inefficiency in light transmission. The system  150  includes an incoming light source  152  that includes a rectangular shaped light emitting surface  154 . The light from the light emitting surface is transmitted through a fiber bundle  156  that includes a circular end surface  158 . In this example, the circular end surface  158  is larger in area than the square shaped light emitting surface  154  and therefore the fiber  154  is only partially illuminated by the light from the light source  152 . The grid sections of the light emitting surface  158  in  FIG. 1A  represent the portion of the fiber optic bundle that is not illuminated by the light source  152 . 
       FIG. 2  is a cross section view of a lighting system  200  including a light guide  202  according to the concepts described herein.  FIG. 3  is a perspective view of the light guide  202 . The light guide  202  in this example is inserted between a light source  204  that has a rectangular light emitting surface  206  and a light receiver such as a fiber optic bundle  208  that includes a circular receiving surface  210 . The light guide  202  has a rectangular interface surface  220  on one end and a circular interface surface  222  on the opposite end. The light guide  202  is free formed and accepts light from the rectangular light emitting surface  206  of the light source  204  and outputs light in a circular shape to the circular receiving surface  210  of the light receiver  208 . The rectangular shaped surface  220  and the circular shaped surface  222  are connected by a free formed surface  224  that transitions from a rectangular cross section to a circular cross section along its length. The light guide  208  can be a solid part of glass, quartz, polymeric material (plastic, silicones, etc) or fused fiber. Light enters the rectangular end surface  220  from the light source  204 , bounces between the free formed surface  224  due to total internal reflection (TIR) and exits the circular end surface  222 . 
     In this example, the light guide  202  is placed close to the light emitting surface  206 , creating an air gap  226 . Some light sources are LEDs having silicone filled domes or flat windows on the light emitting surface  206 . When the light guide  202  is closer to the light source  204 , more light can be collected and transmitted to the light receiver  208 . The circular shaped surface  210  of the light receiver  208  can be placed directly against the light guide as shown in  FIG. 2  or with a small air gap. Alternatively, the light receiver  208  may be absent so the circular surface  222  of the light guide  202  outputs light directly from the light source  204 . Alternatively, the circular shaped surface  222  of the light guide  202  may be coupled to a lens or a reflector instead of the light receiver  208 . 
     Either end surface  220  or  222  of the light guide  202  or both may be coated with wavelength filtering or/and anti-reflection film. The light guide  202  may be doped with color to achieve certain spectral characteristics. The light source  204  may be an LED that emits a single color or several colors. Thus the light guide  202  efficiently mixes different colors when the light source emits several colors. For example, a 4-chip LED comprising a red, a green, a blue and a white chip may be mixed into white light of a different color temperature by the light guide  202 . By the free form surface  224 , the light guide  202  wastes no light when the receiver surface is circular. Thus about 20% more light is delivered to the receiver in the case of the light guide  202  serving as an interface in the case of the components in  FIG. 1A . Correspondingly, the entirety of the light receiver is used in the case of the light guide  202  serving as an interface in the case of the components in  FIG. 1B . 
       FIGS. 4A-4D  show the various dimensions of the light guide  202  in  FIGS. 2-3 .  FIG. 4A  shows the dimensions of the cross section of light guide.  FIG. 4B  shows the dimensions of the rectangular end surface  220 .  FIG. 4C  shows the dimensions of the free formed surface  224  along the line  4 A- 4 A′ of  FIG. 4A .  FIG. 4D  shows the dimensions of the circular end surface  222 . 
     The free formed surface  224  connecting the rectangular surface  220  and the circular surface  222  may be expressed in following formula. For the rectangular end surface  220  of the light guide  202  with length a and width b as shown in  FIG. 4B , any points on this end may be expressed in cylindrical coordinates as (φ 1 , r 1 , z 1 ), where 
                   {             φ1   =       (       -     arctan   ⁡     (     b   /   a     )         ,     arctan   ⁡     (     b   /   a     )         )     ⋁     (       π   -     arctan   ⁡     (     b   /   a     )         ,                       π   +     arctan   ⁢     (     b   /   a     )         )                 r   ⁢           ⁢   1     =     a          2   ⁢   cos   ⁢           ⁢   φ                          z   ⁢           ⁢   1     =   0           ⁢     
     ⁢   or             (     4   ⁢     -     ⁢   1     )               {           φ1   =       (       arctan   ⁡     (     b   /   a     )       ,     π   -     arctan   ⁡     (     b   /   a     )           )     ⋁     (       π   +     arctan   ⁡     (     b   /   a     )         ,                         -   arctan     ⁢     (     b   /   a     )       )                 r   ⁢           ⁢   1     =     a          2   ⁢   sin   ⁢           ⁢   φ                          z   ⁢           ⁢   1     =   0                   (     4   ⁢     -     ⁢   2     )               
The rectangle is divided into four sections.
 
     For the circular end surface  222  of the light guide  202  with radius R, any points on the circular end surface  222  may be expressed as (φ 2 , r 2 , z 2 ), where 
                   {             φ   ⁢           ⁢   2     =     (     0   ,     2   ⁢   π       )                   r   ⁢           ⁢   2     =   R                 z   ⁢           ⁢   2     =   L                   (     4   ⁢     -     ⁢   3     )               
Along the length (axis Z), the free formed surface  224  is a collection of points P=(φ, r, z). Since the radius, r, gradually changes from r 1  to r 2  relative to z as shown in  FIG. 4A , r can be derived from r 1 , r 2  and z. Thus point P can be expressed as
 
                   {           φ   ⁢           =     (     0   ,     2   ⁢   π       )                 r   =           (     r   ⁢           ⁢   1     )     ⁢     (     L   -   z     )       +       (     r   ⁢           ⁢   2     )     ⁢     (   z   )         L                 z   =     (     0   ,   L     )                     (     4   ⁢     -     ⁢   4     )               
Replacing r 1 , r 2  with previous equations (4-1), (4-2), (4-3), leads to
 
     
       
         
           
             
               
                 
                   { 
                   
                     
                       
                         
                           
                             φ 
                             = 
                             
                               
                                 ( 
                                 
                                   
                                     - 
                                     
                                       arctan 
                                       ⁡ 
                                       
                                         ( 
                                         
                                           b 
                                           / 
                                           a 
                                         
                                         ) 
                                       
                                     
                                   
                                   , 
                                   
                                     arctan 
                                     ⁡ 
                                     
                                       ( 
                                       
                                         b 
                                         / 
                                         a 
                                       
                                       ) 
                                     
                                   
                                 
                                 ) 
                               
                               ⋁ 
                               
                                 ( 
                                 
                                   
                                     π 
                                     - 
                                     
                                       arctan 
                                       ⁡ 
                                       
                                         ( 
                                         
                                           b 
                                           / 
                                           a 
                                         
                                         ) 
                                       
                                     
                                   
                                   , 
                                 
                               
                             
                           
                         
                       
                       
                         
                           
                             
                               π 
                               + 
                               
                                 arctan 
                                 ⁢ 
                                 
                                   ( 
                                   
                                     b 
                                     / 
                                     a 
                                   
                                   ) 
                                 
                               
                             
                             ) 
                           
                         
                       
                       
                         
                           
                             r 
                             ⁢ 
                             
                                 
                             
                             = 
                             
                               
                                 
                                   a 
                                   ⁡ 
                                   
                                     ( 
                                     
                                       L 
                                       - 
                                       z 
                                     
                                     ) 
                                   
                                 
                                 + 
                                 
                                   
                                      
                                     
                                       2 
                                       ⁢ 
                                       cos 
                                       ⁢ 
                                       
                                           
                                       
                                       ⁢ 
                                       φ 
                                     
                                      
                                   
                                   ⁢ 
                                   
                                     ( 
                                     
                                       R 
                                       - 
                                       z 
                                     
                                     ) 
                                   
                                 
                               
                               
                                 
                                    
                                   
                                     2 
                                     ⁢ 
                                     cos 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     φ 
                                   
                                    
                                 
                                 ⁢ 
                                 L 
                               
                             
                           
                         
                       
                       
                         
                           
                             z 
                             = 
                             
                               ( 
                               
                                 0 
                                 , 
                                 L 
                               
                               ) 
                             
                           
                         
                       
                     
                     ⁢ 
                     
                       
 
                     
                     ⁢ 
                     or 
                   
                 
               
               
                 
                   ( 
                   
                     4 
                     ⁢ 
                     
                       - 
                     
                     ⁢ 
                     5 
                   
                   ) 
                 
               
             
             
               
                 
                   { 
                   
                     
                       
                         
                           φ 
                           = 
                           
                             
                               ( 
                               
                                 
                                   arctan 
                                   ⁡ 
                                   
                                     ( 
                                     
                                       b 
                                       / 
                                       a 
                                     
                                     ) 
                                   
                                 
                                 , 
                                 
                                   π 
                                   - 
                                   
                                     arctan 
                                     ⁡ 
                                     
                                       ( 
                                       
                                         b 
                                         / 
                                         a 
                                       
                                       ) 
                                     
                                   
                                 
                               
                               ) 
                             
                             ⋁ 
                             
                               ( 
                               
                                 
                                   π 
                                   + 
                                   
                                     arctan 
                                     ⁡ 
                                     
                                       ( 
                                       
                                         b 
                                         / 
                                         a 
                                       
                                       ) 
                                     
                                   
                                 
                                 , 
                               
                             
                           
                         
                       
                     
                     
                       
                         
                           
                             
                               - 
                               arctan 
                             
                             ⁢ 
                             
                               ( 
                               
                                 b 
                                 / 
                                 a 
                               
                               ) 
                             
                           
                           ) 
                         
                       
                     
                     
                       
                         
                           r 
                           ⁢ 
                           
                               
                           
                           = 
                           
                             
                               
                                 a 
                                 ⁡ 
                                 
                                   ( 
                                   
                                     L 
                                     - 
                                     z 
                                   
                                   ) 
                                 
                               
                               + 
                               
                                 
                                    
                                   
                                     2 
                                     ⁢ 
                                     sin 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     φ 
                                   
                                    
                                 
                                 ⁢ 
                                 
                                   ( 
                                   
                                     R 
                                     - 
                                     z 
                                   
                                   ) 
                                 
                               
                             
                             
                               
                                  
                                 
                                   2 
                                   ⁢ 
                                   sin 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   φ 
                                 
                                  
                               
                               ⁢ 
                               L 
                             
                           
                         
                       
                     
                     
                       
                         
                           z 
                           ⁢ 
                           
                               
                           
                           = 
                           
                             ( 
                             
                               0 
                               , 
                               L 
                             
                             ) 
                           
                         
                       
                     
                   
                 
               
               
                 
                   ( 
                   
                     4 
                     ⁢ 
                     
                       - 
                     
                     ⁢ 
                     6 
                   
                   ) 
                 
               
             
           
         
       
     
     The free-formed surface  224  is fully defined by the parameters a, b, R, L. At an arbitrary position z along the length, the section of the light guide  202  looks like something between a rectangle and a circle as shown in  FIG. 4C . 
     Alternatively, the rectangular end can be a square shape. The equations (4-1) and (4-2) become: 
                   {               φ   ⁢           ⁢   1     =       (         -   45     ⁢   °     ,     45   ⁢   °       )     ⋁     (       135   ⁢   °     ,     225   ⁢   °       )                     r   ⁢           ⁢   1     =     a          2   ⁢   cos   ⁢           ⁢   φ                          z   ⁢           ⁢   1     =   0           ⁢     
     ⁢   or             (     4   ⁢     -     ⁢   7     )               {             φ   ⁢           ⁢   1     =       (       45   ⁢   °     ,     135   ⁢   °       )     ⋁     (       225   ⁢   °     ,       -   45     ⁢   °       )                     r   ⁢           ⁢   1     =     a          2   ⁢   sin   ⁢           ⁢   φ                          z   ⁢           ⁢   1     =   0                   (     4   ⁢     -     ⁢   8     )               
The square is equally divided into four sections.
 
     Sometimes, a light guide of a circular end is not feasible to manufacture, so a regular polygon shape  500  as shown in  FIG. 5  may be in place to approximate the circle. Still in the cylindrical coordinate, the regular polygon  500  of N sides circumscribed by a circle of radius R may be expressed as: 
     
       
         
           
             
               
                 
                   { 
                   
                     
                       
                         
                           
                             
                               φ 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               2 
                             
                             = 
                             
                               ( 
                               
                                 0 
                                 , 
                                 
                                   2 
                                   ⁢ 
                                   π 
                                 
                               
                               ) 
                             
                           
                         
                       
                       
                         
                           
                             
                               
                                 r 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 2 
                               
                               = 
                               
                                 
                                   
                                     R 
                                     in 
                                   
                                   
                                      
                                     
                                       cos 
                                       ( 
                                       
                                         φ 
                                         - 
                                         
                                           
                                             ( 
                                             
                                               n 
                                               - 
                                               1 
                                             
                                             ) 
                                           
                                           ⁢ 
                                           α 
                                         
                                       
                                        
                                     
                                   
                                 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 or 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 
                                   
                                     R 
                                     in 
                                   
                                   
                                      
                                     
                                       cos 
                                       ⁡ 
                                       
                                         ( 
                                         
                                           φ 
                                           - 
                                           
                                             
                                               ( 
                                               
                                                 n 
                                                 - 
                                                 1 
                                               
                                               ) 
                                             
                                             ⁢ 
                                             α 
                                           
                                           - 
                                           
                                             α 
                                             / 
                                             2 
                                           
                                         
                                         ) 
                                       
                                     
                                      
                                   
                                 
                               
                             
                             , 
                           
                         
                       
                       
                         
                           
                             
                               n 
                               = 
                               1 
                             
                             , 
                             2 
                             , 
                             
                               3 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               … 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               N 
                             
                           
                         
                       
                       
                         
                           
                             
                               z 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               2 
                             
                             = 
                             L 
                           
                         
                       
                     
                     ⁢ 
                     
                       
 
                     
                     ⁢ 
                     Where 
                   
                 
               
               
                 
                   ( 
                   
                     4 
                     ⁢ 
                     
                       - 
                     
                     ⁢ 
                     9 
                   
                   ) 
                 
               
             
             
               
                 
                   { 
                   
                     
                       
                         
                           
                             R 
                             in 
                           
                           = 
                           
                             R 
                             
                               cos 
                               ⁡ 
                               
                                 ( 
                                 
                                   α 
                                   / 
                                   2 
                                 
                                 ) 
                               
                             
                           
                         
                       
                     
                     
                       
                         
                           α 
                           = 
                           
                             4 
                             ⁢ 
                             
                               π 
                               / 
                               N 
                             
                           
                         
                       
                     
                   
                 
               
               
                 
                   ( 
                   
                     4 
                     ⁢ 
                     
                       - 
                     
                     ⁢ 
                     10 
                   
                   ) 
                 
               
             
           
         
       
     
     Although preferred embodiments have been depicted and described in detail herein, it will be apparent to those skilled in the relevant art that various modifications, additions, substitutions, and the like can be made without departing from the spirit of the invention and these are therefore considered to be within the scope of the invention as defined in the claims which follow.