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Publication numberUS3132812 A
Publication typeGrant
Publication dateMay 12, 1964
Filing dateAug 29, 1961
Priority dateAug 29, 1961
Publication numberUS 3132812 A, US 3132812A, US-A-3132812, US3132812 A, US3132812A
InventorsStrobel Howard E
Original AssigneeEastman Kodak Co
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Flash reflector with improved corner illumination
US 3132812 A
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Description  (OCR text may contain errors)

y 12, 1954 H. E. STROBEL 3,132,812

FLASH REFLECTOR WITH IMPROVED CORNER ILLUMINATION Filed Aug. 29, 1961 HOWARD E. STROBEL INVENTOR.

By IE WM WM/MI,

ATTORNEYS United States Patent Filed Aug. 29, 1961, Ser. No. 134,703 3 Claims. (Cl. 240-41.35)

This invention relates to reflectors for use with flash or flood lamps.

It is the object of the invention to provide a reflector which gives substantially uniform illumination over a square or rectangular area and which does so efliciently. Prior attempts have been made to illuminate a square or rectangular area for photography. When this has involved the shape of the reflector back of the light source, it has been done by bending the corners of the reflector outward to direct more light to the corners of the rectangle or square. Such an arrangement involves a larger than normal reflector and defeats in part the main purpose of the recent trend toward smaller and smaller flash lamps. Thus the specific object of the present invention is to provide as compact a reflector as is reasonable which is still capable of directing extra light to the corners of the square or rectangle to be illuminated.

In the present invention this is done by making the areas of the reflector which are located coplanar with the diagonals of the field to be illuminated, more convex and effectively closer to the light source than the other areas. That is, the areas on the diagonal are moved inward rather than outward so that these areas reflect the light from an axially located source, back across the axis of the reflector to the opposite corners of the field. Such a system is operative whether the base of the lamp extends through an axial hole in the reflector or extends radially in front of or through a marginal hole in the reflector. However, it is most convenient with the simple axial mounting of the flood or flash lamp and it will therefore be described with reference to such a simple mounting of the lamp.

According to the invention a cup shaped reflector having a square symmetry about its axis, consists of four approximately spherical but preferably toric or ellipsoidal sections as described in detail below. The light from the Whole system including the lamp and the reflector, diverges in an approximately square pyramid with rounded dihedral edges. That is, the divergent light has a cross section which is a square with rounded corners and has more or less uniform luminous flux over the area of this approximate square. It should be noted that the square corresponding to the cross section of this divergent light is oriented at 45 to the square of symmetry of the cup shaped reflector; the accompanying drawings illustrate the orientation.

With a simple figure of revolution either a sphere, paraboloid or ellipsoid, the illumination over a square area utilizing a high proportion of the total light, falls off toward the corners of the square to about /5 the value at the center. This corresponds to about 2.3 aperture stops of a camera lens. While such variation is often tolerated, it is, of course, quite objectionable.

The use of exact figures in describing the distribution of illumination must either be over-simplified or must become so complicated to gain precision, that the meaning becomes obscured. Actually the intensities or bright- 3,132,812 Patented May 12., 1964 to concentrate the light on the scene being photographed without wasting any more than is absolutely necessary on other areas, the rate of fall off takes a very sharp dip at some angle (say 39) trom the axis. The square area to be illuminated normally has its corners outside or just at this limiting angle and has the centers of the sides of the square inside the cone thus formed. In such a case the brightness at the corners is about Ms to the brightness at the center of the sides of the square. The present invention by sending more light to the corners rather than to the center of the field, brings the illumination at the corners up to a value approximately equal to that of the centers of the sides of the square and above half that at the center of the square itself. Thus the difference in intensity between the center of the square and the corners is the equivalent of less than one aperture stop which is rarely if ever objectionable and the illumination around the periphery of the square is more or less constant.

The actual distribution of illumination depends on the precision with which the flash lamp or filament of the flood lamp is located with respect to the reflector. Flash bulbs are commonly located accurately to within {-1- or .t)l inch. One of the advantages and objects of the present invention is the 'fact that the positioning of the lamp is not as critical as it is with a spherical or ellipsoidal reflector. of each section away from the section so that the light reflected is approximately collimated (slightly diverging) as it travels back across the axis to the opposite corner of the field. That is, each section of the reflector reflects =a diverging cone whose axis crosses the axis of the whole reflector. f

The invention will be more fully understood from the following description when read in connection with the accompanying'drawings in which:

FIG. 1 geometrically indicates the manner in which the reflector according to theinvention is generated mathematically.

FIG. 2 similarly illustrates a comparison of two sections of a reflector so generated.

FIG. 3 is a perspective view of as shown in FIG. 1.

FIG. 4 is a diagram to illustrate the operation of the reflector.

FIGS. 5 and 6 are respectively front and sectional views of a reflector according to the invention.

FIGS. 1 to 4 are geometrical illustrations and are described in terms of cutting, combining etc. for clarity. In actual practice the reflectors are made by simply the reflector generated molding and coating. The terms used in describing the nesses which should be compared, are the intensity at geometric generation of the shape required are purely figurative.

In FIG. 1, one end of an ellipsoid is cut so that two central sections bounded respectively by planes 10 and 11 are cut away leaving only segments 12, -13, 14 and 15. The center sections which are removed are shown quite wide, since this best illustrates the effect of the present invention. It is, however, exaggerated, and in practice only a somewhat narrower horizontal and vertical section are absent (geometrically removed). A side view of sections 1'3 and 14 appears to the right as 13' and 14 and similar views of sections 13 and 15. appear to the lower right as 13" and 15," of FIG; 1.

If superimposed, these sections would appear as shown in FIG. 2. When the four sections are combined (compacted) a complete reflector is formed as shown in FIG. 3. In none of these first three figures is any provision made for the lamp. The lamp may be supported from the front and held at the proper axial location'in which case the cup shape reflector remains intact as shown in FIGS. 3 and 4. Alternatively, a hole may be pro- The lamp is approximately at the focal length vided through one or more of the reflector segments so that the lamp may be supported through the hole. The operation of the present invention does not depend on the manner in which the lamp is supported, but it does depend on where it is located.

As shown in FIG. 4 the reflector made up of segments 12, 13, 14 and has a square symmetry about the axis 20. The diagonals of the square of symmetry are vertical and horizontal coplanar with the dividing lines between the segments of the reflector. Light from a lamp located on the axis radiates in all directions, some of it going directly to the scene to be illuminated. Part of it travels in the opposite direction and is reflected back toward the scene diverging just enough to cover the angular field of view of the camera, but not enough to waste light to the sides. a This gives generally uniform illumination at the scene but in order to efficiently illuminate a square area, the reflecting surface 12 reflects more light toward the area 22 which constitutes a corner of the square 21 to be illuminated. Similarly the reflector segment 13 tends to concentrate the light in area (or direction) 23, the segment 14 tends to concentrate the light in area (or direction) 24 and the segment 15 tends to concentrate light in the area (or direction) 25. Thus emitting from the lamp and its reflector is a divergent pyramid of light whose cross section or isolumen line (see below) is an approximate square 21 with rounded corners. There is of course some light outside of this pyramid and there is some variation of intensity within the pyramid, but the square 21 more or less identifies the limit of useful illumination.

One can consider light directly from the lamp, i.e. without reflection as forming the core of the divergent pyramid of light and extending outside the pyramid so that some of the direct light is wasted. Because of the edges of the cup shaped reflector, there is a tendency for more of this direct light to be lost beyond the sides of the square 21 than beyond the corners. However, the direct light is not as important as the reflected light. Thus the diverging pyramid of light is primarily made up of the four diverging cones respectively from the four segments and the axes of the cones cross the axis of the reflector itself. The circles of illumination (centered at 22, 23, 24 and 25) probably overlap considerablyand each actually extends across the axis of the reflector. However, these circles 22, 23, 24 and 25 are shown as confined to their own corners, for the sake of clarity. In any case, the light from the lamp and cup shaped reflector does form a diverging pyramid of light with rounded dihedral edges and the light for these dihedral edges comes primarily from the segment of the reflector on the opposite side of the axis.

It is repeated that the light does not fall to zero intensity at the boundary 21, and the light in each of the four cones from the reflector segments does not fall to zero intensity at the broken circles 22, 23, 24 and 25. These illustrated lines can be considered as isolux or isolumen lines, although they are only approximately so; Also the rate of change of intensity is quite rapid near these particular isolumen lines. Inside the lines, the light is intense and more or less uniform. Outside the lines, the light falls rapidly to low intensity not useful for photography illumination.

It should be noted that the centers of the segments 12, 13, 14 and 15 lie on the diagonals of the square field 21 to be illuminated. That is, the square of symmetry of the reflector is'at 45 to the square of the diverging pyramid of light.

The geometry and operation of the invention have been described with respect to an ellipsoid compacted according to the invention. The invention operates with a sphere similarly compacted or preferably with an approximately spherical toroidal or prolate spheroid section. It should be obvious that the center of curvature of each segment (or the equivalent center of curvature if the segment is not a perfect sphere) falls beyond or on the opposite side of the axis. For a definition of opposite side one may refer to FIG. 6 discussed in detail below and note that the axis of the reflector is a horizontal center line (not drawn in) and that the surface 30, for example is on one side of this axis and its center of curvature 41 is not on the same side of the axis, it is on the opposite side of the axis. or zone is used a major curvature is coplanar with the axis of the reflector and the center of this major curvature is on the opposite side of the axis. The lamp on the axis is not located exactly at the focal point of each segment since this would mean that the light reflected would be approximately perfectly collimated and not properly diverging. The lamp is slightly closer to the reflector than the focal point is. It is just inside the focal point which is about /2 the distance from the segment to its center of curvature.

An actual reflector according to the present invention which has proven to be particularly eflicient is illustrated in FIGS. 5 and 6. The segments 30, 31, 32 and 33 with an axially located hole 34 are shown with the dividing lines such as 35 clearly identified. However, in practice the reflectors are molded of plastic and the dividing lines 35 are rounded ofl. so that they are not apparent. A flash lamp 413 is inserted from the front into a socket 43 in the usual way commonly used in flash lamps. The point 41 represents the approximate center of curvature of the reflector segment 30 and the point 42 similarly represents the approximate center of curvature of the segment 32 of the reflector. If the reflector were a complete surface of revolution (perfectly spherical surface), 41 and 42 would coincide and would lie on the axis of the reflector. The displacement of each of the centers 41 and 42 from the axis is a measure of the amount by which the segment of the reflector is geometrically compacted or pushed toward the center by the removal of center sections. This displacement of the center of curvature from the axis is therefore a measure of the amount of increase of light to the corners of the picture. The dis placement is usually between 7 and 20% of the radius of curvature itself and is preferably about 12%. The distance of the effective location of the lamp 40 from the centers 41 and 42 is slightly greater than half the distance of the centers from the reflectors. If it were exactly half, the reflected light from each segment would be collirnated forming a hot spot at each corner. Thus one is easily able to increase the light to the corners to a value greater than required, which means that one may select between the extremes, any distribution desired. As mentioned above it is preferable to select one giving approximately uniform illumination around the square periphery with about double intensity at the center of the square. That is the effective distance of the lamp from the reflector should preferably be between one-third and one-half the effective radius of the reflector.

Having thus described preferred embodiments of my invention I wish to point out that it is not limited thereto but is of the scope of the appended claims.

I claim:

1. A cup shaped reflector in combination with means for holding a light source at a point on the axis thereof to produce a diverging light beam shaped as an approximately square pyramid with rounded dihedral edges, said reflector consisting of four approximately spherical sections concave to the axis and symmetrically located on the diagonals of said pyramid and each section being located with its center of curvature beyond the axis and over twice and less than three times as far from the reflector as said point on the axis to divergingly reflect a portion of the light from the source back across the axis to form the opposite rounded dihedral edge of said pyramid.

2. A reflector according to claim 1 in which said ap When a toroid section References Cited in the file of this patent UNITED STATES PATENTS Clark Dec. 4,

Halvorson Apr. 30,

Smith et all. June 13,

De Graff Oct. 31,

FOREIGN PATENTS Great Britain June 28,

France June 22,

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US1248456 *Sep 6, 1916Dec 4, 1917Paul L ClarkProjection-machine illumination.
US1711478 *Mar 18, 1925Apr 30, 1929Gen ElectricLight reflector
US1913519 *Jan 25, 1933Jun 13, 1933Harry E BuffingtonLight projector
US3007035 *Oct 24, 1958Oct 31, 1961Groff Kenneth C DePhotographic light source
FR365302A * Title not available
GB276030A * Title not available
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3321620 *Aug 5, 1963May 23, 1967Linear IncSolar simulator
US3331960 *Nov 27, 1964Jul 18, 1967Sylvania Electric ProdPortable photogrpahic light
US3423582 *Jan 3, 1967Jan 21, 1969Sylvania Electric ProdLighting unit
US4229782 *Dec 20, 1977Oct 21, 1980Mcgraw-Edison CompanyHigh efficiency lighting units with beam cut-off angle
US5823662 *Aug 25, 1994Oct 20, 1998Lightware, Inc.In an imaging system
Classifications
U.S. Classification362/297
International ClassificationF21V7/00, G03B15/03, G02B5/08, G03B15/04, F21V7/04
Cooperative ClassificationG02B5/08, G03B15/0442, F21V7/04
European ClassificationG02B5/08, G03B15/04D, F21V7/04