US3702395A

US3702395A - Condenser system for high intensity light source

Info

Publication number: US3702395A
Application number: US79416A
Authority: US
Inventors: Gottfried R Rosendahl
Original assignee: US Department of Navy
Current assignee: US Department of Navy
Priority date: 1970-10-09
Filing date: 1970-10-09
Publication date: 1972-11-07
Anticipated expiration: 1989-11-07

Abstract

An elliptical mirror is utilized in combination with a xenon arc projection lamp and a high melting point metal stop to provide in one embodiment an improved vertical axis point light source for point light source projectors, and in another embodiment to provide a condensed, vertical axis beam which is annular in section for panoramic projectors using transparencies having an azimuthal scene recorded in annular form.

Description

United States Patent Rosendahl [451 Nov. 7, 1972 [541 CONDENSER SYSTEM FOR HIGH INTENSITY LIGHT SOURCE [72] Inventor: Gottfried R. Rosendahl, Park,Fla.

[73] Assignee: The United States of America as represented by the Secretary of the Navy [22] Filed: Oct. 9, 1970 [21] App1.No.: 79,416

Winter [52] US. Cl. ..240/4l.3, 353/97, 353/102 [51] Int. Cl ..F2lv 13/04 [58] Field of Search ..240/41.3, 41.35, 41; 353/55,

[56] References Cited UNITED STATES PATENTS 3,598,989 8/1971 Biggs ..240/4l.3 X 1,838,312 12/1931 Kanolt ..355/133 3,457,012 7/1969 Ucko et a1. ..355/78 3,321,620 5/1967 Miles et a1 ..240/41.3 1,279,638 9/1918 Blake ..240/41.3 3,174,067 3/1965 Bahrs ..353/55 X 3,078,760 2/1963 Brownscombe.....240/4l.35 R

3,241,440 3/1966 Kugler ..240/41.3 X 2,338,901 l/l944 Chiti ..240/4l.3 3,371,202 2/1968 Moore et a1. ..240/4l.3 X 3,590,239 6/1971 Bernard ..240/41 .3

FOREIGN PATENTS OR APPLICATIONS 1,012,820 7/1957 Germany ..240/41 R OTHER PUBLICATIONS That Important Optical Train International Projectionist, Vol. 32, No. 2, February 1957 Primary ExaminerSamuel S. Matthews Assistant Examiner-Richard M. Sheer Attorney-Richard S. Sciascia, John W. Pease and Harvey A. David [5 7] ABSTRACT An elliptical mirror is utilized in combination with a xenon arc projection lamp and a high melting point metal stop to provide in one embodiment an improved vertical axis point light source for point light source projectors, and in another embodiment to provide a condensed, vertical axis beam which is annular in section for panoramic projectors using transparencies having an azimuthal scene recorded in annular form.

1 Claim, 3 Drawing Figures Fri/yarn 45 6/07 14 4/ foe/re Pro 'erf/an y: em

minimum 1 m2 3.702.395

sum 2 0F 2 FIG.3

Op/ics FIG.2

GOTTFRIED R. RQSENDAHL wvavme CONDENSER SYSTEM FOR HIGH INTENSITY LIGHT SOURCE STATEMENT OF GOVERNMENT INTEREST The invention described herein may be manufactured and used by or for the Government of the United States of America for governmental purposes without the payment of any royalties thereon or therefor.

BACKGROUND OF THE INVENTION Various projection and display devices require a high intensity light source. One commonly used high intensity light source is the xenon arc lamp. Use of the xenon arc projection lamp has been limited to use with condenser arrangements wherein the direction of light propagation from the projector is generally horizontal. The construction of xenon projection lamps is characterized by a glass envelope having a bulbous central portion and diametrically opposed tubular portions extending therefrom. Tungsten electrodes define a gap within the bulbous portion of the envelope while elongated electrode supporting and conductive leads extend in opposite directions through the tubular portions. The electrodes, gap, and electrode supporting leads all lie on a common axis. These lamps are required to be operated with the axis of the electrodes disposed in a vertical or nearly vertical position.

Operating the lamps with the electrode axis vertical is satisfactory for applications using condenser systems following the conventional approach wherein the condensed light beam axis is in a horizontal direction. There are, however, applications which require a condensed light beam which has a vertical axis. The requirement of a vertical light beam axis contradicts the usual requirement that a xenon arc lamp be burned with the electrode axis vertical, provided the condenser system follows the conventional approach. It will be appreciated that this is so inasmuch as the tubular portions of the envelope, as well as the electrode supports or leads and the electrodes themselves, obstruct the efficient emission of light in a vertical sense.

Additionally, light sources such as the xenon arc lamp are generally characterized by light emission from a rather small luminous area; and within this area the luminance is strongly non-uniform. These characteristic features are contrasted by, for instance, the pure carbon or high intensity (so called Beck) arc lamp and require special attention in the form of carefully adapted condenser systems, in order to utilize the light to the highest possible degree without compromising uniformity of screen illumination within acceptable standards. Xenon arc lamps have been used to some degree in combination with an elliptical reflector in schlieren projection systems. In those systems, typified by the conventional projection system produced by the Dojun Koki Co. of Japan, it is desired to provide even illumination over a relatively wide field, whereas the instant invention is concerned mainly with a combination which will provide an effective point light source.

In the art of simulators and trainers there is a need with a panoramic or around the horizon projection system utilizing an annular transparency and requiring a vertical axis condenser system and illumination of a cone between 25 and from the condenser axis.

SUMMARY OF THE INVENTION With the foregoing in mind, it is a principal object of this invention to provide, in combination with a projection lamp (such as a xenon lamp) which requires burning in an approximately vertical position, a condenser system which will utilize the light emitted around the entire equatorial zone and brought out in the direction of the longitudinal axis of the lamp, that is in a vertical direction.

As another object the present invention aims to provide an improved light source or condenser arrangement utilizing a generally elliptical mirror having a central opening for accommodating a vertically extending, elongated portion of a projection lamp, the mirror having first and second focal points along the vertical axis thereof, the light emitting portion of the lamp being centered at the first focal point, and a stop or lens being located at the second focal point.

Still another object of this invention is the provision of a light source and condenser of the foregoing character which is relatively simple and inexpensive to manufacture and to align or adjust, and which compensates for a rather large source of emission and which is aspherical in shape.

BRIEF DESCRIPTION OF THE DRAWINGS Other objects and advantages of the invention will become apparent from the following detailed description when read in conjunction with the accompanying sheet of drawings forming a part of this specification, and in which:

FIG. 1 is a diagrammatic illustration of an improved, vertical axis condenser system embodying the present invention, showing the same as used in conjunction with a point light source projection system;

FIG. 2 is a graphical illustration showing the relationship between a stop element of the system of FIG. 1 and the illumination in the plane of that stop element; and

FIG. 3 is a diagrammatic illustration of another embodiment of the invention as used with panoramic pro jection system.

DESCRIPTION OF THE PREFERRED EMBODIMENTS In the form of the invention which is illustrated in FIG. 1 in association with a point light source projection system 10, there is provided a xenon arc projection lamp 12. The lamp 12 is of conventional construction including a transparent envelope 14 having diametrically opposed tubular portions 14a, 14b having their long axes arranged vertically, or substantially so. These axes may be said to define the vertical axis 15 of the lamp 12. A tungsten electrode or anode 16 is supported by a lead 18 which extends vertically through the tubular portion 14a. A tungsten electrode or cathode 20 is supported by a lead 22 which is axially aligned with the lead 18 and extends through the tubular portion 14b. The envelope is filled with the gas xenon at a number of atmospheres pressure. Upon an appropriate starting pulse, and thereafter with a direct current voltage on the order of 200-volts applied via lines L and L, across the

leads

18 and 22,-a bell shaped arc A is established and maintained between the electrodes 16 and 20. The are A emits an intense white light, suitable for projection, through the side walls of the envelope 14.

Surrounding the projection lamp 12 is an elliptical concave mirror 30 having an inner reflecting surface 32 which constitutes a portion of a surface of revolution about an axis which is coincident with the vertical axis of the lamp 12. The elliptical mirror has a central aperture or opening 34 through which the bulb portion 14a extends-and is configured so that afirst focal point F thereof is located at the center of the arc A, while the second or remote focal pointF is located along the axislS at a substantial distance below the lamp l2.

' There results from the aforedescribed combination of the lamp 12 and the elliptical mirror 30 a conical zone of occlusion which subtends an angle a, and a zone of illumination which subtends a maximum angle b. The elliptical mirror 30 is selected to have the focal point F far enough down the axis 15 that the ratio of the angle a to the angle b is approximately as 25 is to 85, or 0.295.

The rays 40 emanating horizontally from the are A will beanastigmatic in their reflection and mergence at the remote focal point F These rays may be considered the central or chief rays of the unoccluded part of the illumination cone. The resulting image of the are A, if formed by the chief rays 40 alone, would also be free of spherical aberrations. However, rays outside the chief rays, such as

rays

42 and 44, will be subject to astigmatism. There will also be coma present in the image at F These aberrations maybe compensated for in the lens system 46 which serves principally to render a reduced and better defined image A of the are A, which will better serve as essentially a pin-point light source for projecting .a scene, recorded on a transparency 48, through the projection system 10. The lens system 46 follows well known principles for a lens triplet and need not be described in detail.

In order to prevent stray light from entering the system and degrading the quality of the image A, an aperture 50 of diameter D is defined by a stop member 52 arranged in the plane of the focal point F Since a large amount of heat is produced at F the stop member 52 is advantageously formed of a high melting point metal such as tantalum or titanium. As is illustrated by curve 54 in FIG. 2 the intensity of illumination in the plane of the stop member 52 and second focal point F is characterized by a plateau, the width of which is determinative of the diameter D of the aperture 50.

A particular advantageof the described system over a conventional imaging system is that the light distribution in the image at F has rotational symmetry, thus overcoming the conventional strong non-uniformity of the arc image in a conventional system. r

Referring nowto FIG. 3, in which reference numerals corresponding to those in the foregoing description identify corresponding parts, there is illustrated another embodiment of the invention which is shown in conjunction with panoramic projection means including a'transparency 60 and panoramic projection optics 62. The transparency 60 and o tics 62 form no part of the invention per se. Sufficert 0 say that n the pro ection system with which this embodiment of the invention is most advantageously used, the transparency 60 comprises an' azimuthal scene recorded in annular form, and when properly illuminated the optics 62 project the scene onto a suitably curved screen 64.

In this embodiment, the lamp 12 and elliptical mirror 30 are substantially the same as described earlier. However, the lens means 46 and stop member 52 are replaced by a negative lens means 68 deployed ahead of the focal point F The lens means 68 serves to defocus the converging rays-represented by 40, 42, and 44 and to form them into parallel rays. The resulting light constitutes a condensed beam 70 of light which is annular in section in that it surrounds a central occluded zone 72. I y Again, stray light is excluded by an aperture 74 defined .by a stop member .76. The light beam 70 of annular section is of a size to correspond to the annularly recorded scene on the transparency 68, thereby obtaining the most efficient use of the light output of the lamp l2.

Obviously many modifications and variations of the present invention are possible in the light of the above teachings. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as specifically described.

What is claimed is: I I 1. In a vertical axis condenser system for use with high intensity light source such as a xenon arc lamp:

a portion of an annular, concave, ellipsoidal mirror having a central opening concentric with the major axis of said mirror; 1

said mirror being disposed with said major axis vertically oriented, and said mirror having first and second focal points on said axis, said I first and second focal points being adjacent and remote, respectively, with respect to said mirror;

said mirror being disposed about a high intensity light source with the light source at said first focal point, said mirror projecting rays of light emitted by the light source into a cone of illumination which forms a first image of the source at said second focal point and a cone of occlusion within said cone of illumination;

said first image being characterized by a high intensity central portion;

stop means formed of high melting point material disposed in a plane extending through said second focal point and normal to said axis, said stop means having an aperture therein with its center on said axis said aperture having a diameter D which limits the passage of light from the light source to the high intensity central portion of said first image; and I lens means disposed beyond said second focal point having its rear focal point at said second focal point and operative to form a reduced second image at a third focal point along said axis, said reduced second image being only of the light transmitted by said aperture whereby said reduced second image is effective as a point light source for use in point light source projection means.

Claims

1. In a vertical axis condenser system for use with a high intensity light source such as a xenon arc lamp: a portion of an annular, concave, ellipsoidal mirror having a central opening concentric with the major axis of said mirror; said mirror being disposed with said major axis vertically oriented, and said mirror having first and second focal points on said axis, said first and second focal points being adjacent and remote, respectively, with respect to said mirror; said mirror being disposed about a high intensity light source with the light source at said first focal point, said mirror projecting rays of light emitted by the light source into a cone of illumination which forms a first image of the source at said second focal point and a cone of occlusion within said cone of illumination; said first image being characterized by a high intensity central portion; stop means formed of high melting point material disposed in a plane extending through said second focal point and normal to said axis, said stop means having an aperture therein with its center on said axis said aperture having a diameter D which limits the passage of light from the light source to the high intensity central portion of said first image; and lens means disposed beyond said second focal point having its rear focal point at said second focal point and operative to form a reduced second image at a third focal point along said axis, said reduced second image being only of the light transmitted by said aperture whereby said reduced second image is effective as a point light source for use in point light source projection means.