The present invention relates to a lamp-and-reflector combination, particularly for projectors, and especially for projectors for amateur-type motion-picture film, transparencies, and the like. The structure and arrangement is, however, also applicable to projection lamps for other uses.
Background.
Modern projection lamps are frequently combined with a reflector into a single unit. One type of lamp which is particularly suitable for use with projectors is a halogen incandescent lamp. It can be used, for example, for projection of 8 mm motion-picture film with a ground glass.
The profile of the reflector of such combination lamp-reflector units may result in imaging of the filament of the incandescent lamp if the filament is very small and has a high primary winding pitch, while the picture window itself is large, and the image-forming objective has a relatively small aperture. If the projection structure is of this kind, localized non-uniformities in the illumination may result. The uniformity of the projection surface of the first order, also known as the G1 uniformity, and so defined in industrial standard DIN 15 148, provides a suitable definition for the basic illumination across a diagonal of the imaging plane. This first-order uniformity may be unaffected by the concurrence of the aforementioned conditions. The uniformity of second order, which may also be termed cloud formation, is, however, disturbed.
It has previously been proposed--see German Pat. No. 1,203,116--to provide a discontinuous profile for the reflector. This was done in order to improve the uniformity of first order. As proposed, the reflector is formed as a composite of a plurality of reflective plane surface areas, located with respect to each other at different angles. The inclination of the respective surface regions is so selected that the images of the filament which are reflected thereby in the vicinity of the optical axis are spaced apart to a greater extent than these images removed from the optical axis, that is, near the periphery. All images of the filament are adjacent each other. The filament images which are projected by different surface areas do not coincide.
The Invention.
It is an object to provide a combination lamp-reflector in which the aforementioned localized irregularities in illumination of the projection surface, e.g. the ground glass, do not occur. Thus, the uniformity of illumination of second order also will be maintained.
Briefly, in accordance with the invention, the profile of the reflector is discontinuous. The reflector is formed by areal segments in the form of conical surfaces, which are successively placed on the reflector at different angles with respect to the reflector axis. Each of these areal segments has a length, within the discontinuous profile of the reflector, which is so dimensioned that the overall length of the projection of the reflected filaments of the lamp, in the plane of the image field or window, is equal or larger than the image field diagonal. Adjacent areas intersect in the discontinuous reflector profile in points which are on a curve which represents a continuous theoretical profile of the reflector, which theoretical, continuous profile follows a known and standard curve.
Forming the reflector as a series of conical surfaces results in projection of a bundle of projected images of the filament in the imaging plane or plane of the window such that the respective images of the filament, within the bundle of images, are offset with respect to height; all the bundles of the images of the filaments commonly overly the imaging plane at the imaging window.
Drawings
FIG. 1 is a vertical sectional view through a lamp-reflector combination using a halogen incandescent lamp with a generally ellipsoid reflector; and
FIG. 2 is an enlarged detail schematic view of the discontinuous profile of the reflector of the lamp-reflector combination of FIG. 1.
A halogen cycle incandescent lamp 1 has a filament 2 and is assembled to a reflector 3 to form a single structural unit--see FIG. 1. As best seen in FIG. 2, the reflector 3 has a discontinuous reflector profile P. The reflector profile P is formed by areal or surface segments F.sub.1, F.sub.2, F.sub.3, F.sub.4. Each one of the areal or surface segments is shaped in the form of a truncated cone-shaped shell, sequentially placed on the reflector at a respectively different angle with respect to the axis or center line CL of the lamp and reflector. Each one of the surface sections F has a length l. The respective lengths l of the surfaces preferably differ. The length l of any surface F is a function of the length of the filament, as seen from the film window and reflected by the reflector, see FIG. 2, and the image rays there shown.
The dimension l is so arranged that the length of the imaged filament in the plane of the film window is not substantially less, preferably of equal size or larger than the diagonal of the image field. Adjacent surface regions F intersect at points B, C, D. These intersecting points--or, rather, intersecting circles in three dimensions--form, in cross section and as seen in FIG. 2, points on a curve K. The curve K is a continuous curve, representative of a continuous reflector profile, which is well known as such, and used for projection purposes. It may, for example, be a continuous reflector profile of a known halogen ellipsoid reflector lamp, and referred to above. Each surface area F projects, thus, a bundle of images of the filament of the lamp towards the plane of the image window in such a manner that the respective separate images of the filaments within the bundle are offset in a vertical direction--see FIG. 2. All the bundles of the images of the filaments commonly or together cover the plane of the film window, superimposed above each other.
In a preferred form, thirteen surface regions F are used. The length l of the respective surface regions, as seen in FIG. 2, decreases to 1.15 mm adjacent the rim of the reflector. The intersecting points--with respect to the cross-sectional view of FIG. 2--of adjacent surfaces are placed on a curve K which is defined by the equation:
The length l at the apex is about 1.73 mm.