Abstract:
A series of highly-reflective contiguous conical segments about an optic  s. The length of each segment side and the cone vertex angle of each cone is related to the overall desired size of the reflector, and the desired angle of radiation from the reflector.

Description:
The invention described may be manufactured, used, and licensed by the U.S. Government for governmental purposes without the payment of any royalties thereon. 
    
    
     BACKGROUND OF THE INVENTION 
     This invention is in the field of electromagnetic reflectors, and is particularly concerned with beam-shaping reflectors for optical radiation (light). Such reflectors are used to produce a collimated or other shaped beam from a point source, or may be used to focus collimated or other rays. Typical examples of the shapes of such reflectors are spherical, parabolic, and arrays of plane reflectors. U.S. Pat. No. 52,987 of Mar. 6, 1866 is an example of such a reflector. In order to produce a beam of a certain divergence from a point source, to which the invention is specifically directed, the usual ways are to employ an aperature in the source housing, or to employ a parabolic reflector with the source at the focus of the reflector and with an aperature to define the desired beam. The chief disadvantage with these ways is that only a portion of the light from the source falls in the desired beam. Obviously, one might employ the combination of a parabolic reflector to collimate all of the light from the source and a diverging lens to yield the desired beam angle. This combination is both more complex (two elements) and more expensive (parabolic reflector) than the inventive reflector, which uses only conic sections. 
     SUMMARY OF THE INVENTION 
     The invention is a reflector of point-source electromagnetic radiation which provides a predetermined solid cone of radiation, and the method for constructing such a reflector. The cone includes all of the radiation from the source, with a substantially uniform radiation flux in a cross-sectional area of the cone. The reflector is made of joined conical sections of different cone angles. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 shows a cross-sectional view of a reflective surface made in accordance with the invention. 
     FIG. 2 shows a cross-sectional view of an inventive reflector with typical rays shown. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     The invention may be best understood if this description is taken in conjunction with the drawing. Referring to FIG. 1, the general shape, and some of the construction of a reflector mode in accordance with the invention, is shown. It is assumed that a point source of radiation will be placed at the optical center on the drawing. From this center, an arc, with a radius R 1  of approximately the length of the desired reflector, is drawn. An optic axis is drawn through the point and the arc, and line segments S1 are drawn, each segment subtending an angle .sup.θ /4 with the optic axis. As shown on the drawing, the upper end of each S1 intersects the arc at the same place that each R 1  does, and the angle between each R 1  and the optic axis .sup.θ /2. Thus, the angle between the R 1  &#39;s is θ, wherein θ is the desired angle of radiation from the source. The lower end of each S1 is the point at which a ray from the optical center is reflected parallel to the S1 on the opposite side of the optic axis. Such a ray is shown as dashed line 10. If a ray were drawn from the optical center to the upper end of S1, this ray would be reflected parallel to the optic axis (see FIG. 2). The upper ends of line segments S2 join segments S1 at their lower ends, and segments S2 have lengths and angles with respect to the optic axis such that a ray from the lower end of S2 will be reflected parallel to the S2 on the opposite side of the optic axis. The angle φ of each S2 and each subsequent S with respect to the optic axis are predetermined in acordance with the following formula: ##EQU1## wherein i is associated with the segment number Si such as S1, S2, etc., up to segment Sn, and n=(360°/θ)-1. If 360/θ 
     is not an integer, the length of Sn will be a fraction of the value of a calculated Sn. The length of R2, R3, or Ri may be calculated from the following formula: ##EQU2## wherein θ is now exprressed in radians as a function of π, and i is a positive integer. 
     The general expression for the length of Si is as follows: ##EQU3## 
     FIG. 2 shows a cross-sectional view of a reflector made in accordance with the invention, with typical rays shown from source (incandescent light bulb) 20 (with power leads 21). As can be seen, the ray impinging on the upper end of each Si segment is reflected parallel to the optic axis, and the ray impinging on the lower end thereof is reflected parallel to the section of Si on the opposite side of the optic axis. 
     Although the various Si&#39;s are shown as line segments, it should be understood that the actual reflector is composed of conical segments. The reflector may be made by any one of various techniques, all well known in the art. For example, it might be made by turning on a numerically controlled lathe, or by cutting sheet metal developments of the segments and bending these developments into shape. If plastic rather than metal is used, it would obviously be necessary to metalize the plastic to provide a highly reflective surface.