Abstract:
The invention concerns a technique for routing an optical fiber through a bend so that it can traverse a hinge or other mechanical connector having a bend radius smaller than the minimum bend radius of the fiber. Particularly, the radius of curvature of an optical fiber traversing a bend can be maximized by routing the fiber so as to have a route component parallel to the axis about which the fiber must bend. For instance, in a hinged connection in which the optical fiber must bend around the axis of the hinge, the optical fiber may be routed over the arc around the hinge with a route component parallel to the axis of the hinge.

Description:
FIELD OF THE INVENTION 
       [0001]    The invention pertains to optical fibers. More specifically, the invention pertains to the routing of optical fibers over curved paths. 
       BACKGROUND OF THE INVENTION 
       [0002]    The use of optical fibers to transmit data over long distances is well known. However, optical fibers are now also being increasingly used to carry signals over very short distances within individual electronic devices due to their extremely large bandwidth and ability to carry large amounts of data over a single fiber in both directions simultaneously. Accordingly, the use of optical fibers for carrying signals in portable devices, such as laptop computers, mobile phones, video cameras, still cameras, personal digital assistants, and portable digital music players, is increasing. 
         [0003]    Many electronic devices, particularly portable ones, for which minimizing their size is a significant design goal, employ mechanisms for folding parts of the device upon each other or sliding parts of the device relative to each other to expand or contract the profile of the device as needed. 
         [0004]    Examples of such devices abound, including flip phones, video cameras with fold out video screens, laptop computers with fold up monitors, and cell phones with slide-out keyboards or displays. 
         [0005]    Generally, at least some circuits within a first part of the device that on one side of a hinged or sliding connection have to electronically communicate with circuits in another part of the device on the other side of the hinge or sliding mechanical connection. 
         [0006]    Accordingly, signal lines must cross such moveable mechanical connection means, such as hinges and sliding connections. Such requirements present some design difficulties in terms of creating a flexible and/or moveable electrical signal path that can survive repeated bending, flexing, translation or other movement. When copper wires are used to transmit signals across such mechanical hinges or other moveable mechanisms, the radius of any bends in the wires typically is not a problem since a copper wire can be bent to virtually any radius without any significant impact on its signal transmission quality. 
         [0007]    However, this is not true of optical fibers. Optical fibers can break if bent to a very small radius. Furthermore, with respect to most optical fibers, their ability to transmit light is substantially compromised long before they reach the physical breaking point radius. More specifically, if an optical fiber is bent too sharply, light traveling in the core of the fiber can actually escape through the cladding and be lost. 
         [0008]    Most optical fibers in use today have a minimum bend radius of about 20 to 25 millimeters. Some optical fibers are now available with minimum bend radii as small as 15 millimeters and it is believed that optical fibers will soon be available with minimum bend radii as small as 10 millimeters. However, such minimum bend radii are still larger than desired for many applications. 
       SUMMARY OF INVENTION 
       [0009]    The invention concerns a technique for routing an optical fiber through a bend so that it can traverse a hinge or other mechanical connector having a bend radius smaller than the minimum bend radius of the fiber. Particularly, the radius of curvature of an optical fiber traversing a bend can be maximized by routing the fiber so as to have a route component parallel to the axis about which the fiber must bend. For instance, in a hinged connection in which the optical fiber must bend around the axis of the hinge, the optical fiber may be routed over the arc around the hinge with a route component parallel to the axis of the hinge. 
     
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         [0010]      FIG. 1A  is a perspective view illustrating an optical fiber of the prior art in a flat, unbent state. 
           [0011]      FIG. 1B  is a perspective view of the optical fiber of the prior art of  FIG. 1A  folded over on itself about a bend radius of r. 
           [0012]      FIG. 1C  is a top plan view of the folded fiber of  FIG. 1B . 
           [0013]      FIG. 1D  is a side plan view of the folded fiber of  FIG. 1B . 
           [0014]      FIG. 1E  is a front plan view of the folded fiber of  FIG. 1B . 
           [0015]      FIG. 2A  is a perspective view of a fiber in accordance with the principles of the invention in a flat, unbent state. 
           [0016]      FIG. 2B  is a perspective view of the optical fiber of  FIG. 2A  folded over on itself about a bend radius of r. 
           [0017]      FIG. 2C  is a top plan view of the folded fiber of  FIG. 2B . 
           [0018]      FIG. 2D  is a side plan view of the folded fiber of  FIG. 2B . 
           [0019]      FIG. 2E  is a front plan view of the folded fiber of  FIG. 2B . 
           [0020]      FIG. 3  is a view of the optical fiber of  FIGS. 2A-2E  in a flat, unbent state illustrating the effective bend radius of the optical fiber. 
           [0021]      FIG. 4  is a perspective view of how the optical fiber of  FIGS. 2A-2E  might bend in association with a sliding mechanical connection. 
           [0022]      FIG. 5  is a perspective view of an alternative embodiment of an optical fiber in a flat, unbent state in accordance with the principles of the present invention. 
           [0023]      FIG. 6A  is a perspective view of a fiber optic ribbon cable in accordance with the principles of the present invention. 
           [0024]      FIG. 6B  is a perspective view of the fiber optic ribbon cable of  FIG. 6A  folded over on itself to the bend radius is r. 
           [0025]      FIG. 6C  is a top plan view of the fiber optic ribbon cable of  FIG. 6B . 
           [0026]      FIG. 6D  is a side plan view of the fiber optic ribbon cable of  FIG. 6B . 
           [0027]      FIG. 6E  is a front plan view of the fiber optic ribbon cable of  FIG. 6B . 
       
    
    
     DETAILED DESCRIPTION 
       [0028]      FIGS. 1A through 1E  illustrate the routing of an optical fiber  10  about a curve in a conventional manner.  FIG. 1A  is a perspective view of the optical fiber  10  in a flattened state (i.e. before it is routed through the curve).  FIG. 1B  is a perspective view of the same fiber after it has been routed around an axis, a, within a radius r of axis a.  FIGS. 1C ,  1 D and  1 E are top, side, and front plan views of the fiber of  FIG. 1B  from perspectives C-C, D-D, and E-E, respectively, in  FIG. 1B . In  FIG. 1A , an imaginary sheet  12  is shown defining a plane within which the optical fiber lies when unbent. Of course, in its flattened state, the optical fiber lies in an infinite number of potential planes and we have merely chosen one of them for illustrative purposes. This sheet  12  also is shown in the views of  FIGS. 1B through 1E  for visual reference purposes to help understand the drawings and the invention. Furthermore, a lengthwise segment  13  of the sheet  12  corresponding to the lengthwise segment of the fiber  10  that is bent is shown in cross hatching in all the drawings to further help with the understanding of the drawings and the invention. 
         [0029]    As can be seen in  FIGS. 1A-1E , if a conventional optical fiber  10  must be capable of bending about an axis a, such as a hinge mechanism of a flip phone, the radius r of the curvature of the optical fiber  10  around that axis  11  must be kept greater than the minimum bend radius of the fiber. 
         [0030]      FIGS. 2A-2E  illustrate an optical fiber routed in accordance with the principles of the present invention. The drawing  FIGS. 2A through 2E  correspond to the same views as  FIGS. 1A through 1E , respectively. That is,  FIG. 1A  is a perspective view illustrating the optical fiber in an unbent state;  FIG. 2B  is a perspective view of the optical fiber bent around axis a with the fiber remaining within a radius r of axis a.  FIGS. 2C ,  2 D, and  2 F are top, side, and front plan views, respectively of the folded fiber of  FIG. 2B . Finally, sheet  22  corresponds to sheet  12  in  FIGS. 1A-1E . 
         [0031]    As can be seen in the Figures, the longitudinal portion of the inventive fiber  20  that bends around the axis a has been given a lateral component in addition to its radial component around the axis a. Referring to the coordinate system shown in  FIGS. 2A-2E , the radial component is the component of curvature in the xy plane, which is a curve of radius r about the axis a. The lateral component is the fiber route component in the z direction. It should be apparent from the Figures, and particularly  FIG. 2B , that the fiber  20  remains within a radius r of axis a (i.e., the radial component of curvature about the axis  21 , i.e., perpendicular to the z axis, is r). However, the effective bend radius experienced by the fiber  20  is much greater than r. In the embodiment of  FIGS. 2A through 2E , the path of the fiber  20  in the longitudinal segment in which it is curved around the axis a (i.e., the cross hatched area  23 ) comprises a substantially straight line (see  FIG. 2A ), i.e., the lateral route component is substantially monotonic. This is merely exemplary, as the path need not necessarily be a straight line. However, if it is a straight line, then the effective bend radius of the fiber  20  over segment  23  is easily calculable via the Pythagorean theorem. Particularly, referring to  FIG. 3 , which is similar to the flattened view of the fiber of  FIG. 2A , but with additional reference data, the bend radius around the axis  21  has previously been defined as r (i.e., the bent longitudinal segment of the fiber remains within r of the axis). That makes the diameter 2r. Let us call the length of the lateral component (in the z direction) of the fiber route l. Thus, we know from the Pythagorean Theorem that the sum of the squares of the sides of a right triangle is equal to the square of the hypotenuse. Therefore: 
         [0000]      (2 r ) 2   +l   2 =(2′) 2  
 
         [0000]    where r′ is the effective bend radius of the optical fiber. Stated another way: 
         [0000]    
       
         
           
             
               r 
               ’ 
             
             = 
             
               
                 
                   
                     ( 
                     
                       2 
                        
                       r 
                     
                     ) 
                   
                   2 
                 
                 + 
                 
                   1 
                   2 
                 
               
               2 
             
           
         
       
     
         [0032]    Note that the curvature of the fiber at the transition areas  25  and  26  should be gradual so as not to exceed the minimum bend radius of the fiber in these areas. Also, note that the equations above are approximations since they do not factor in the fact that the fiber route in area  23  is not actually perfectly straight, but includes some curvature in areas  25  and  26 . 
         [0033]      FIG. 4  illustrates the same optical fiber  20  as in  FIGS. 2A-2E , but showing how it might bend in association with a sliding mechanical connection, in which the imaginary sheet  22  would bend into an S-shaped curve (rather than the U-shaped curve of  FIGS. 2B-2E ). 
         [0034]    As just noted, the monotonic lateral component illustrated in the embodiment of  FIGS. 2A-2E  is merely exemplary. Other shapes are possible also. For instance,  FIG. 5  is a view of an alternate optical fiber in its flat state illustrating another possible route. 
         [0035]      FIGS. 6A-6E  are a series of views similar to the view of  FIGS. 1A-1E , respectively, or  2 A- 2 E, respectively, of a ribbon cable  60  constructed in accordance with the principles of the present invention. It is possible to fabricate ribbon cables, foils, flexible printed circuit boards, etc. employing the principles of the present invention in which other, non-optical signal conductors, such as copper wires and copper coaxial conductors also are embedded. Thus, for instance, in the ribbon cable of  FIGS. 6A-6E , some of the signal conductors  61  may be optical fibers, but others may be copper or other electrically conductive conductors. 
         [0036]    In the flat state shown in the view of  FIG. 6A , the ribbon cable  60  comprises a plurality of signal conductors  61  laid out side by side so as to form the ribbon  60  having first and second longitudinal ends  65 ,  66  and first and second parallel opposing major surfaces  68 ,  69  with the signal conductors running the longitudinal extent of the ribbon between the first and second ends  65 ,  66 . 
         [0037]    The ribbon  60  runs substantially in a longitudinal direction, x. However, longitudinal segment  63  of the ribbon  60  includes a path component in direction z; parallel to the first and second opposing major surfaces and transverse to the primary longitudinal direction x of the ribbon. 
         [0038]    Thus, with reference to  FIG. 7 , describing the fiber paths in more geometric terms, we can consider a ribbon cable to define an imaginary surface  70 , namely, the surface that contains the centers of all of the fibers in the cable. The aforementioned two parallel opposing major surfaces  68 ,  69  of the ribbon  60  are parallel to this surface  70 . When the ribbon cable is laid flat, surface  70  is substantially planar. However, when the cable is curved, the surface  70  is commensurately curved. We can consider that, within this surface  70 , there are two dimensions. Let us define the direction corresponding to the direction between the longitudinal ends of the ribbon cable as the x direction and the direction corresponding to the direction between the two parallel edges  61 ,  62  of the ribbon cable as the y direction. In a conventional ribbon cable, the fiber paths have a directional component only in one direction, the x direction. However, in a ribbon cable incorporating the present invention, at least a portion of the fiber paths have a component in the y direction also. 
         [0039]    While  FIGS. 6A-6E  illustrate an embodiment of a ribbon cable in which the entire cable  60  has a transverse path component, this is merely exemplary. In yet other embodiments such as illustrated in  FIG. 8 , which shows another ribbon cable  80  in its flat state, the ribbon cable  80  itself could remain entirely straight, while a longitudinal segment  86  of the optical fibers  81  within the ribbon cable  80  include a path component transverse the longitudinal axis of the ribbon. 
         [0040]    The principles of the invention also can be employed in connection with optical fibers embedded in flexible printed circuit boards (which may include both copper and optical fiber conductors). 
         [0041]    Similarly, the principles of the invention may be employed in connection with interconnections between different layers of a multi layer printed circuit board or between two parallel-mounted printed circuit boards. 
         [0042]    Having thus described a few particular embodiments of the invention, various alterations, modifications, and improvements will readily occur to those skilled in the art. Such alterations, modifications and improvements as are made obvious by this disclosure are intended to be part of this description though not expressly stated herein, and are intended to be within the spirit and scope of the invention. Accordingly, the foregoing description is by way of example only, and not limiting. The invention is limited only as defined in the following claims and equivalents thereto.