US3449561A - Aconic collector - Google Patents

Aconic collector Download PDF

Info

Publication number
US3449561A
US3449561A US650703A US3449561DA US3449561A US 3449561 A US3449561 A US 3449561A US 650703 A US650703 A US 650703A US 3449561D A US3449561D A US 3449561DA US 3449561 A US3449561 A US 3449561A
Authority
US
United States
Prior art keywords
source
collector
axis
aconic
energy
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US650703A
Inventor
Richard W Basil
Frederic N Benning
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Textron Electronics Inc
Original Assignee
Textron Electronics Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Textron Electronics Inc filed Critical Textron Electronics Inc
Application granted granted Critical
Publication of US3449561A publication Critical patent/US3449561A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V7/00Reflectors for light sources
    • F21V7/04Optical design
    • F21V7/08Optical design with elliptical curvature

Definitions

  • a light collecting mirror for directing radiant energy from a source such as an arc lamp onto a given area wherein the shape of the collecting reflector is such as to compensate for finite source size of the radiant energy to provide a desired uniform illuminance on the area or, if desired, provide a predetermined graded illuminance.
  • the collector is formed by revolving about a generating axis curved line segments which constitute in part portions of ellipses whose major axes lie at different acute angles to the generating axis.
  • the secondary foci of the ellipses are thus radially spaced from the generating axis so that ring patterns are formed at the area illuminated.
  • a series of concentric rings of decreasing radii may be provided in the test area with the result of fairly uniform illuminance. Further uniformity and compensation is achieved by having some of the secondary foci fall beyond the plane of the test area such that the images provided at the test area serve to fill in desired darker portions to provide the uniform illuminance.
  • This invention relates generally to energy collecting and directing surfaces and more particularly, to a novel collector for directing energy from a source onto a given area to provide a desired illuminance on any test object positioned in said given area.
  • Energy collecting surfaces are well known in the art and generally take the form of an ellipsoid.
  • a source of energy is placed at one focus and a test body having a given area to be irradiated is positioned at the conjugate focus.
  • all of the energy from the source will be directed to the conjugate focus.
  • the given area to be irradiated is of substantial size, there will be lacking a uniform or desired gradation of illuminance of the body.
  • an ellipsoid collector necessarily directs energy from the source to the conjugate focal point, there will develop a hot spot at this particular point.
  • part of the energy is Wasted in overconcentration at one point and underconcentration at adjacent areas.
  • light energy sources do not constitute point sources and as a result, the refocussed energy is distributed in a manner corresponding to the geometry of the light source itself. Since this geometry is not uniform, there is again presented the problem of a nonuniformly irradiated area.
  • An aconic surface may be defined briefly as a surface of revolution generated by revolving a curved line segment which, in itself, may or may not constitute part of a conic section, about a given straight line axis different from the axis of the particular curved line segment if such happens to constitute a portion of a conic section.
  • the aconic collector surface is defined by revolving a curved line segment about a straight line axis passing through the source and the center of the given area to be irradiated.
  • This curved line segment constitutes a portion of an ellipse having a first focus coincident with the source and its conjugate focus lying in a plane normal to the referred to straight line axis, the major axis of the ellipse forming an acute angle with the straight axis.
  • the plane includes the given area to be irradiated.
  • the conjugate focus of the ellipse will describe a ring when a source is placed at the focus of the resulting aconic surface. There will thus be provided a distribution of energy following a ring about the center of the given area.
  • a plurality of curved line segments successively connected together may be caused to rotate about a given straight line axis passing through the source and the center of a given area to be irradiated.
  • These successive curved line segments may constitute portions of a series of ellipses all having their first foci coincident with the source and their conjugate foci successively radially spaced from the center of the given area as a consequence of having their major axes successively inclined at varying acute angles with respect to the straight line axis.
  • the resulting aconic collector surface will distribute energy in a pattern of concentric rings so that the energy from the source is fairly uniformly distributed over the given area.
  • the illuminance of the given area may be graded so that certain areas will receive more radiation than other areas.
  • the surface may be designed to compensate for the geometry of a finite light source such as an arc lamp to provide a desired uniformity. Further finite source size compensation may be realized by utilizing segments of ellipses having major axes of different lengths in addition to different angular relationships to the generating axis for the collector.
  • FIGURE 1 is a diagrammatic showing useful in explaining the principles of forming the aconic collector surface of this invention
  • FIGURE 2 is a greatly enlarged portion of the diagram of FIGURE 1;
  • FIGURE 3 illustrates in perspective view a first embodiment of an aconic collector in accordance with the invention
  • FIGURE 4 is a further diagrammatic representation useful in explaining the principles of forming another embodiment of the aconic collector
  • FIGURE 5 is a diagrammatic illustration of the invention including a finite source geometry for which compensation of nonuniformity of the source is realized;
  • FIGURE 6 is a schematic view of the image resulting from the collector of FIGURE 5.
  • FIGURE 1 there is shown an ellipse 10 having a first focus F1 and a conjugate focus F2.
  • the major axis of this ellipse is designated A.
  • an energy source would be positioned at the focus F1 and a target or test body to be illuminated would be positioned at the conjugate focus F2.
  • all of the energy radiated from the source at F1 would be reflected and concentrated at the conjugate focus F2.
  • the collecting surface may be formed by providing a second ellipse indicated at 10.
  • This second ellipse is constructed to have its first focal point F1 coincident with the focal point F1 of the first ellipse 10 and thus be coincident with the position of the source of radiant energy.
  • the major axis of the second ellipse, indicated at A is inclined at an acute angle W to the major axis A of the first ellipse 10.
  • the conjugate focal point F2 of the second ellipse 10 will fall substantially in a plane including the focal point F2 but spaced therefrom, this plane being normal to the major axis A of the first ellipse 10.
  • a segmental portion of the second ellipse 10' is indicated by the heavy line S extending between points M and N. If this curved line segment S is now revolved about the axis A corresponding with the major axis of the first ellipse 10, an aconic surface will be generated.
  • the resulting surface is illustrated at 11 in FIGURE 3.
  • the points M and N will assume the positions M1 and N1 which fall inside a conventional ellipsoid collector formed by the first ellipse 10. If a source of radiant energy 12 is now positioned at the focus P2 of this collector surface 11, the energy will be directed and distributed over a body 13 as indicated by the shaded area 14. This distribution is in the form of a ring having a center corresponding to the center of the given area to be illuminated as indicated by the numeral 15.
  • the axis about which the curved line segment S is caused to revolve corresponds with a straight line axis A passing through the source 12 and the center of the given area 13, the major axis A of the ellipse from which the curved line segment S was derived and described in conjunction with FIGURE 2 being inclined at the acute angle W to the straight line axis A.
  • the aconic collector may be generated from a series of connected curved line segments corresponding to portions of a series of ellipses.
  • FIGURE 4 there is illustrated a series of portions of ellipses 16, 17, 18, and 19 all having a common first focal point F coincident with a desired source of radiant energy (not shown).
  • the major axes of these ellipses indicated at A16, A17, A18 and A19 form successively increasing acute angles starting at zero with respect to a straight line axis passing through the source at focal point F and the center of the body 13.
  • the conjugate focal points of the series of ellipses are spaced at increasing radial distances from the center of the plane of the target area, these conjugate focal points being indicated at F16, F17, F18, and F19.
  • the length of the various curved line segments S16 through S19 may be adjusted prior to generating the surface so that different surface areas for these respective line segments are provided in the composite complete aconic collector thereby resulting in different concentrations of energy from these various segments.
  • the energy distribution over the target area may be graded as desired.
  • FIGURE 5 there is illustrated a further embodiment of the invention wherein there is defined a generating axis AG and a first line segment S21 constituting part of a first ellipse 21 having a first focal point F21 lying on the generating axis AG and a second focal point F21 falling in a plane P1 normal to the generating axis.
  • the second focal point P21 is radially spaced from the generating axis in the plane P1.
  • a second line segment S22 in turn is defined by part of a second ellipse 22 having a first focal point F22 coincident with focal point F21 in a finite source 23.
  • the second focus for the second ellipse 21 is indicated at F22 and lies a given radial distance from the generating axis AG in a second plane P2 spaced from the first plane P1. It will be noted that the major axes of the respective ellipses lie at different acute angles relative to the generating axis AG.
  • the line segments S21 and S22 may be smoothly connected together and are shown in heavy lines in FIG- URE 5. If these two lines are now revolved about the generating axis AG, there will result an aconic collector shown in dashed lines at 24.
  • the particular finite source 23 depicted in FIGURE 5 is for an arc lamp and is designated for simplicity by means of the small arrow and a cooperating electrode.
  • the end of the arrow for the arc lamp constitutes a very intense light source the radiation over the area of the source decreasing towards the spaced electrode.
  • the ring of illuminance at the radial distance 25 from the generating axis AG is shown as greater than the somewhat out-of-focus image of the arrow formed by the segment S21 when viewed in the plane P2.
  • rotation of the images to form the concentric rings results in a fairly uniform illuminance of the area.
  • the generating line segments are defined by ellipses having different length major axes such that the secondary foci may lie in different planes all normal to the generating axis AG but spaced along the generating axis relative to each other.
  • the present invention has provided a greatly improved radiant energy collecting and directing surface structure. Not only is a greater portion of the emitted energy collected as a consequence of the particular form of the aconic surface, but as a consequence of the distribution of the energy over the given area to be irradiated, the energy is efficiently used and the formation of concentrated hot spots and the like as a result of finite sources is wholly avoided.
  • An aconic collector for distributing energy from a source onto a given area in accordance with a predetermined illuminance, comprising, in combination: at least two reflecting surfaces positioned together to form a composite collector generated by revolving at least two curved line segments about a straight line generating axis passing through said source and the center of said given area, said curved line segments constituting portions of at least two ellipses, respectively, having first foci coincident with each other and said source and second foci spaced given distances from said source and at different radial distances from said generating axis, respectively, the major axes of said ellipses forming different acute angles with said straight line generating axis.
  • An aconic collector in which said source is of a finite size to provide nonuniformly irradiating light from different spaced portions on said source, said curved line segments defining said reflecting surfaces when revolved about said generating axis being dimensioned such that said predetermined illuminance on said given area is substantially uniform.
  • An aconic collector according to claim 1 in which the second foci of said ellipses lie substantially in a single plane normal to said generating axis.
  • An aconic collector in which the second foci of said ellipses lie respectively in parallel planes spaced along the generating axis and normal thereto, said given area coinciding with one of said planes.
  • An aconic collector for distributing energy from a source onto a given area in accordance with a predetermined illuminance, comprising, in combination: a series of concave reflecting surfaces connected together to form a composite collector generated by revolving a series of successive curved line segments about a straight line axis passing through said source and the center of said given area, said curved line segments successively constituting portions of a series of ellipses having first foci all coincident with each other and said source and second foci substantially in planes spaced along and normal to said straight line axis, said second foci being spaced at different radial distances in said planes from said straight line generating axis respectively, the major axes of said ellipses forming successively varying acute angles with said straight line axis.

Description

June 10, 1969 R. w. BASIL ET AL ACONIC COLLECTOR Sheet Filed July 5.. 1967 June 10, 1969 R, w, BAS|L ET AL ACONIC COLLECTOR Sheet Filed July 3, 1967 FIG. 5
INVENTORQ RICHARD W. BASIL FREDERIC N. BENNING FIG. 6
ATTORNEYS United States Patent Int. Cl. F21v 7/08 US. Cl. 240-103 Claims ABSTRACT OF THE DISCLOSURE A light collecting mirror for directing radiant energy from a source such as an arc lamp onto a given area wherein the shape of the collecting reflector is such as to compensate for finite source size of the radiant energy to provide a desired uniform illuminance on the area or, if desired, provide a predetermined graded illuminance. The collector is formed by revolving about a generating axis curved line segments which constitute in part portions of ellipses whose major axes lie at different acute angles to the generating axis. The secondary foci of the ellipses are thus radially spaced from the generating axis so that ring patterns are formed at the area illuminated. By using a large number of such segments for generating the collector, a series of concentric rings of decreasing radii may be provided in the test area with the result of fairly uniform illuminance. Further uniformity and compensation is achieved by having some of the secondary foci fall beyond the plane of the test area such that the images provided at the test area serve to fill in desired darker portions to provide the uniform illuminance.
This application is a continuation-in-part of copending application Ser. No. 291,079, filed June 27, 1963, now abandoned and entitled Aconic Collector.
This invention relates generally to energy collecting and directing surfaces and more particularly, to a novel collector for directing energy from a source onto a given area to provide a desired illuminance on any test object positioned in said given area.
Energy collecting surfaces are well known in the art and generally take the form of an ellipsoid. With such a collector, a source of energy is placed at one focus and a test body having a given area to be irradiated is positioned at the conjugate focus. By this arrangement, all of the energy from the source will be directed to the conjugate focus. If the given area to be irradiated is of substantial size, there will be lacking a uniform or desired gradation of illuminance of the body. In other words, since an ellipsoid collector necessarily directs energy from the source to the conjugate focal point, there will develop a hot spot at this particular point. Thus, part of the energy is Wasted in overconcentration at one point and underconcentration at adjacent areas. In many instances, it would be desirable to irradiate a given area fairly uniformly rather than concentrate all of the energy at one particular point.
Further, and as a practical matter, light energy sources do not constitute point sources and as a result, the refocussed energy is distributed in a manner corresponding to the geometry of the light source itself. Since this geometry is not uniform, there is again presented the problem of a nonuniformly irradiated area.
With the foregoing in mind, it is a primary object of this invention to provide a collecting and directing surface capable of distributing energy over a given area in a predetermined manner to the end that hot spots are avoided.
More particularly, it is an object to provide a collector and directing device for distributing energy over a given area so designed that the illuminance of the area may be rendered uniform or graded as desired and in a manner to compensate for the geometry of finite sized light sources.
Briefly, these and other objects and advantages of this invention are realized by avoiding the use of an ellipsoid type reflecting surface and instead employing an aconic surface. An aconic surface may be defined briefly as a surface of revolution generated by revolving a curved line segment which, in itself, may or may not constitute part of a conic section, about a given straight line axis different from the axis of the particular curved line segment if such happens to constitute a portion of a conic section.
In one embodiment of the invention, the aconic collector surface is defined by revolving a curved line segment about a straight line axis passing through the source and the center of the given area to be irradiated. This curved line segment constitutes a portion of an ellipse having a first focus coincident with the source and its conjugate focus lying in a plane normal to the referred to straight line axis, the major axis of the ellipse forming an acute angle with the straight axis. The plane includes the given area to be irradiated. Because of the inclination of the major axis of the ellipse of the curved line segment to the straight line axis about which the curved line segment is revolved to generate the aconic surface, the conjugate focus of the ellipse will describe a ring when a source is placed at the focus of the resulting aconic surface. There will thus be provided a distribution of energy following a ring about the center of the given area.
In other embodiments of the invention, a plurality of curved line segments successively connected together may be caused to rotate about a given straight line axis passing through the source and the center of a given area to be irradiated. These successive curved line segments may constitute portions of a series of ellipses all having their first foci coincident with the source and their conjugate foci successively radially spaced from the center of the given area as a consequence of having their major axes successively inclined at varying acute angles with respect to the straight line axis. The resulting aconic collector surface will distribute energy in a pattern of concentric rings so that the energy from the source is fairly uniformly distributed over the given area. By initially adjusting the relative lengths of the series of curved line segments forming the aconic collector, the illuminance of the given area may be graded so that certain areas will receive more radiation than other areas.
It is evident from the foregoing that the surface may be designed to compensate for the geometry of a finite light source such as an arc lamp to provide a desired uniformity. Further finite source size compensation may be realized by utilizing segments of ellipses having major axes of different lengths in addition to different angular relationships to the generating axis for the collector.
A better understanding of the invention will be had by now referring to preferred embodiments thereof as illustrated in the accompanying drawings, in which:
FIGURE 1 is a diagrammatic showing useful in explaining the principles of forming the aconic collector surface of this invention;
FIGURE 2 is a greatly enlarged portion of the diagram of FIGURE 1;
FIGURE 3 illustrates in perspective view a first embodiment of an aconic collector in accordance with the invention;
FIGURE 4 is a further diagrammatic representation useful in explaining the principles of forming another embodiment of the aconic collector;
FIGURE 5 is a diagrammatic illustration of the invention including a finite source geometry for which compensation of nonuniformity of the source is realized; and,
FIGURE 6 is a schematic view of the image resulting from the collector of FIGURE 5.
Referring first to FIGURE 1, there is shown an ellipse 10 having a first focus F1 and a conjugate focus F2. The major axis of this ellipse is designated A. In conventional ellipsoid type collectors, an energy source would be positioned at the focus F1 and a target or test body to be illuminated would be positioned at the conjugate focus F2. By the properties of the ellipsoid, all of the energy radiated from the source at F1 would be reflected and concentrated at the conjugate focus F2. There would thus develop a concentrated radiation at the point on the object coinciding with the conjugate focus F2 and an underconcentration of energy at adjacent points with the result that the energy would not be used efficiently.
In order to provide a collector in accordance with the present invention which will distribute the energy over a given area at which a target or test body is positioned, the collecting surface may be formed by providing a second ellipse indicated at 10. This second ellipse is constructed to have its first focal point F1 coincident with the focal point F1 of the first ellipse 10 and thus be coincident with the position of the source of radiant energy. However, the major axis of the second ellipse, indicated at A, is inclined at an acute angle W to the major axis A of the first ellipse 10. As a consequence, the conjugate focal point F2 of the second ellipse 10 will fall substantially in a plane including the focal point F2 but spaced therefrom, this plane being normal to the major axis A of the first ellipse 10.
With particular reference to FIGURE 2, a segmental portion of the second ellipse 10' is indicated by the heavy line S extending between points M and N. If this curved line segment S is now revolved about the axis A corresponding with the major axis of the first ellipse 10, an aconic surface will be generated.
The resulting surface is illustrated at 11 in FIGURE 3. As shown, after the curved line segment S has been revolved about the axis A 180 degrees the points M and N will assume the positions M1 and N1 which fall inside a conventional ellipsoid collector formed by the first ellipse 10. If a source of radiant energy 12 is now positioned at the focus P2 of this collector surface 11, the energy will be directed and distributed over a body 13 as indicated by the shaded area 14. This distribution is in the form of a ring having a center corresponding to the center of the given area to be illuminated as indicated by the numeral 15. Thus, the axis about which the curved line segment S is caused to revolve corresponds with a straight line axis A passing through the source 12 and the center of the given area 13, the major axis A of the ellipse from which the curved line segment S was derived and described in conjunction with FIGURE 2 being inclined at the acute angle W to the straight line axis A.
In actual practice, it is not possible to provide a point source of radiant energy. As a result, there will not result a narrow ring of concentrated energy in the plane of the second focus, but rather a broad ring area fairly uniformly illuminated.
To render the distribution even more uniform or even to grade the illuminance on a given area, the aconic collector may be generated from a series of connected curved line segments corresponding to portions of a series of ellipses. Thus, with particular reference to FIGURE 4, there is illustrated a series of portions of ellipses 16, 17, 18, and 19 all having a common first focal point F coincident with a desired source of radiant energy (not shown). The major axes of these ellipses indicated at A16, A17, A18 and A19 form successively increasing acute angles starting at zero with respect to a straight line axis passing through the source at focal point F and the center of the body 13. Thus, the conjugate focal points of the series of ellipses are spaced at increasing radial distances from the center of the plane of the target area, these conjugate focal points being indicated at F16, F17, F18, and F19.
If now given curved line segments are selected from 'these respective ellipses and successively connected together, such as indicated at S16, S17, S18, and S19, there will result an overall curved line segment which may be revolved about the axis A16 corresponding to the straight line axis passing through the focal point F and the center of the target. The resulting aconic collector will then serve to distribute the radiant energy at the focal point F over a pattern described by a plurality of concentric rings such as indicated at 20. Again, because of the actual physical size of the radiation source as opposed to a theoretical point source, a clear definition of concentric rings will not result but generally they will merge into each other to form a relatively uniform distribution of illuminance on the target 13.
In forming the aconic surface as described in FIGURE 4, the length of the various curved line segments S16 through S19 may be adjusted prior to generating the surface so that different surface areas for these respective line segments are provided in the composite complete aconic collector thereby resulting in different concentrations of energy from these various segments. Thus, the energy distribution over the target area may be graded as desired.
Referring now to FIGURE 5, there is illustrated a further embodiment of the invention wherein there is defined a generating axis AG and a first line segment S21 constituting part of a first ellipse 21 having a first focal point F21 lying on the generating axis AG and a second focal point F21 falling in a plane P1 normal to the generating axis. As indicated, the second focal point P21 is radially spaced from the generating axis in the plane P1.
A second line segment S22 in turn is defined by part of a second ellipse 22 having a first focal point F22 coincident with focal point F21 in a finite source 23. The second focus for the second ellipse 21 is indicated at F22 and lies a given radial distance from the generating axis AG in a second plane P2 spaced from the first plane P1. It will be noted that the major axes of the respective ellipses lie at different acute angles relative to the generating axis AG.
The line segments S21 and S22 may be smoothly connected together and are shown in heavy lines in FIG- URE 5. If these two lines are now revolved about the generating axis AG, there will result an aconic collector shown in dashed lines at 24.
The particular finite source 23 depicted in FIGURE 5 is for an arc lamp and is designated for simplicity by means of the small arrow and a cooperating electrode. The end of the arrow for the arc lamp constitutes a very intense light source the radiation over the area of the source decreasing towards the spaced electrode. Thus, considering the tip of the arrow of the source 23, from the first revolved line segment S21, there will result at the second focus F21 an image of the arrow as shown in plane P1.
The image from the second segment S22 of the arrow representing the hot point of the arc lamp source will appear in the plane P2 at F22 as shown in FIGURE 5. In this same plane P2, there will also'be a certain illuminance as a consequence of the first ellipse line segment S21 but this will not quite be in focus because of the spacing of the plane P2 from the focal point F21 in the plane P1. Further, it will be spaced radially closer to the generating axis line AG than the image at the second focus F21 in the plane P1.
It will be evident from the foregoing that as a consequence of the complete reflecting surfaces formed by revolving the line segments S21 and S22 about the generating axis, the resulting ring type images, as they appear in the area defined by the plane P2, will be substantially similar to that illustrated in FIGURE 6.
Referring specifically to FIGURE 6, the ring of illuminance at the radial distance 25 from the generating axis AG is shown as greater than the somewhat out-of-focus image of the arrow formed by the segment S21 when viewed in the plane P2. Thus, rotation of the images to form the concentric rings results in a fairly uniform illuminance of the area.
The only difference between the embodiment illustrated in FIGURES 5 and 6 and that described in conjunction with FIGURE 4 is the fact that the generating line segments are defined by ellipses having different length major axes such that the secondary foci may lie in different planes all normal to the generating axis AG but spaced along the generating axis relative to each other. By this further variation in the refocussing of the collected radiation from the source, a further control over the final illumination in the desired area is realized.
From the foregoing description, it will be evident that the present invention has provided a greatly improved radiant energy collecting and directing surface structure. Not only is a greater portion of the emitted energy collected as a consequence of the particular form of the aconic surface, but as a consequence of the distribution of the energy over the given area to be irradiated, the energy is efficiently used and the formation of concentrated hot spots and the like as a result of finite sources is wholly avoided.
Minor modifications falling clearly Within the scope and spirit of this invention will occur to those skilled in the art. The aconic collector is therefore not to be thought of as limited to the exact embodiments set forth merely for illustrative purposes.
What is claimed is:
1. An aconic collector for distributing energy from a source onto a given area in accordance with a predetermined illuminance, comprising, in combination: at least two reflecting surfaces positioned together to form a composite collector generated by revolving at least two curved line segments about a straight line generating axis passing through said source and the center of said given area, said curved line segments constituting portions of at least two ellipses, respectively, having first foci coincident with each other and said source and second foci spaced given distances from said source and at different radial distances from said generating axis, respectively, the major axes of said ellipses forming different acute angles with said straight line generating axis.
2. An aconic collector according to claim 1, in which said source is of a finite size to provide nonuniformly irradiating light from different spaced portions on said source, said curved line segments defining said reflecting surfaces when revolved about said generating axis being dimensioned such that said predetermined illuminance on said given area is substantially uniform.
3. An aconic collector according to claim 1, in which the second foci of said ellipses lie substantially in a single plane normal to said generating axis.
4. An aconic collector according to claim 1, in which the second foci of said ellipses lie respectively in parallel planes spaced along the generating axis and normal thereto, said given area coinciding with one of said planes.
5. An aconic collector for distributing energy from a source onto a given area in accordance with a predetermined illuminance, comprising, in combination: a series of concave reflecting surfaces connected together to form a composite collector generated by revolving a series of successive curved line segments about a straight line axis passing through said source and the center of said given area, said curved line segments successively constituting portions of a series of ellipses having first foci all coincident with each other and said source and second foci substantially in planes spaced along and normal to said straight line axis, said second foci being spaced at different radial distances in said planes from said straight line generating axis respectively, the major axes of said ellipses forming successively varying acute angles with said straight line axis.
References Cited UNITED STATES PATENTS 1,275,120 8/1918 Ballman et al. 1,756,084 4/1930 Caughlan 24041.37 1,819,725 8/1931 Wood 240-4137 3,028,486 4/1962 Simmon 3251l3 NORTON ANSHER, Primary Examiner.
RICHARD M. SHEER, Assistant Examiner.
US. Cl. X.R. 24041.35
US650703A 1967-07-03 1967-07-03 Aconic collector Expired - Lifetime US3449561A (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US65070367A 1967-07-03 1967-07-03

Publications (1)

Publication Number Publication Date
US3449561A true US3449561A (en) 1969-06-10

Family

ID=24609947

Family Applications (1)

Application Number Title Priority Date Filing Date
US650703A Expired - Lifetime US3449561A (en) 1967-07-03 1967-07-03 Aconic collector

Country Status (1)

Country Link
US (1) US3449561A (en)

Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3529148A (en) * 1967-12-13 1970-09-15 Trw Inc Collector and method for producing a nearly uniform distribution of flux density on a target plane perpendicular to the optical axis
US3689760A (en) * 1971-01-25 1972-09-05 Mattel Inc Efficient reflector for a projector
US3702930A (en) * 1971-03-12 1972-11-14 Olivetti & Co Spa Remote illuminating apparatus
US3707626A (en) * 1970-04-10 1972-12-26 Robert John Delchen Optical reflector
US3763348A (en) * 1972-01-05 1973-10-02 Argus Eng Co Apparatus and method for uniform illumination of a surface
US3786247A (en) * 1968-11-29 1974-01-15 Chicago Aerial Ind Inc Optical illumination system
FR2201425A1 (en) * 1972-09-29 1974-04-26 Optical Radiation Corp
US4010374A (en) * 1975-06-02 1977-03-01 Ppg Industries, Inc. Ultraviolet light processor and method of exposing surfaces to ultraviolet light
US4035631A (en) * 1975-12-15 1977-07-12 General Electric Company Projector lamp reflector
US4149227A (en) * 1977-06-20 1979-04-10 Corning Glass Works Reflector
US4234247A (en) * 1978-10-30 1980-11-18 Corning Glass Works Method of making a reflector
US4320442A (en) * 1979-10-11 1982-03-16 Kollmorgen Technologies Corporation Annular illuminator
DE3212698A1 (en) * 1981-04-14 1982-11-18 Cibie Projecteurs, 93012 Bobigny HEADLIGHTS FOR MOTOR VEHICLES
US4814606A (en) * 1985-11-15 1989-03-21 E. I. Du Pont De Nemours And Company Photodetector assembly for a laser scanning apparatus
FR2623634A1 (en) * 1987-11-25 1989-05-26 Armines INFRARED RADIATION TRANSMITTING APPARATUS COMPRISING A PLANE SOURCE OF INFRARED RADIATION AND A REFLECTOR
US5971569A (en) * 1997-06-11 1999-10-26 Steris Corporation Surgical light with stacked elliptical reflector

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1275120A (en) * 1914-08-06 1918-08-06 Edwin C Ballman Projecting apparatus.
US1756084A (en) * 1928-03-07 1930-04-29 Martha W Caughlan Reflector
US1819725A (en) * 1926-04-05 1931-08-18 American Woodlite Corp Light projecting reflector
US3028486A (en) * 1959-08-17 1962-04-03 Rossi Veikko Radiosonde and temperature controlling means therefor

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1275120A (en) * 1914-08-06 1918-08-06 Edwin C Ballman Projecting apparatus.
US1819725A (en) * 1926-04-05 1931-08-18 American Woodlite Corp Light projecting reflector
US1756084A (en) * 1928-03-07 1930-04-29 Martha W Caughlan Reflector
US3028486A (en) * 1959-08-17 1962-04-03 Rossi Veikko Radiosonde and temperature controlling means therefor

Cited By (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3529148A (en) * 1967-12-13 1970-09-15 Trw Inc Collector and method for producing a nearly uniform distribution of flux density on a target plane perpendicular to the optical axis
US3786247A (en) * 1968-11-29 1974-01-15 Chicago Aerial Ind Inc Optical illumination system
US3707626A (en) * 1970-04-10 1972-12-26 Robert John Delchen Optical reflector
US3689760A (en) * 1971-01-25 1972-09-05 Mattel Inc Efficient reflector for a projector
US3702930A (en) * 1971-03-12 1972-11-14 Olivetti & Co Spa Remote illuminating apparatus
US3763348A (en) * 1972-01-05 1973-10-02 Argus Eng Co Apparatus and method for uniform illumination of a surface
FR2201425A1 (en) * 1972-09-29 1974-04-26 Optical Radiation Corp
US4010374A (en) * 1975-06-02 1977-03-01 Ppg Industries, Inc. Ultraviolet light processor and method of exposing surfaces to ultraviolet light
US4035631A (en) * 1975-12-15 1977-07-12 General Electric Company Projector lamp reflector
US4149227A (en) * 1977-06-20 1979-04-10 Corning Glass Works Reflector
US4234247A (en) * 1978-10-30 1980-11-18 Corning Glass Works Method of making a reflector
US4320442A (en) * 1979-10-11 1982-03-16 Kollmorgen Technologies Corporation Annular illuminator
DE3212698A1 (en) * 1981-04-14 1982-11-18 Cibie Projecteurs, 93012 Bobigny HEADLIGHTS FOR MOTOR VEHICLES
US4814606A (en) * 1985-11-15 1989-03-21 E. I. Du Pont De Nemours And Company Photodetector assembly for a laser scanning apparatus
FR2623634A1 (en) * 1987-11-25 1989-05-26 Armines INFRARED RADIATION TRANSMITTING APPARATUS COMPRISING A PLANE SOURCE OF INFRARED RADIATION AND A REFLECTOR
EP0318390A1 (en) * 1987-11-25 1989-05-31 Association Pour La Recherche Et Le Developpement Des Methodes Et Processus Industriels (Armines) Electromagnetic ray emitter apparatus, particularly for infrared, comprising a planar source and a reflector
US4922107A (en) * 1987-11-25 1990-05-01 A.R.M.I.N.E.S. Apparatus emitting an electromagnetic radiation, in particular infrared, comprising a plane source of rays and a reflector
US5971569A (en) * 1997-06-11 1999-10-26 Steris Corporation Surgical light with stacked elliptical reflector

Similar Documents

Publication Publication Date Title
US3449561A (en) Aconic collector
US4683525A (en) Lamp having segmented reflector
US1248456A (en) Projection-machine illumination.
US2492946A (en) Pattern density ray approximating reflector
US3453425A (en) Structure for concentrating radiant energy
US4035631A (en) Projector lamp reflector
JPH05501924A (en) Optical lenses and related equipment
US3522424A (en) Searchlight apparatus
US3529148A (en) Collector and method for producing a nearly uniform distribution of flux density on a target plane perpendicular to the optical axis
US1887650A (en) Light controlling apparatus
US3732417A (en) Square lite projector using prismatic lens
US2297124A (en) Lighting fixture
AU600312B2 (en) Lighting apparatus
US4355350A (en) Reflector for use in an artificial lighting device
JPS6125123Y2 (en)
RU2047876C1 (en) Device for light-beam treatment
US2771001A (en) Optical illumination system with homogeneous distribution of light for projectors
US3398272A (en) Isoradiant energy reflecting
US3588493A (en) Projecting lamps having reflector which form rectangular patterns of light
US1880892A (en) Light projection apparatus
US3513306A (en) Multimodular collimated light projection system
IE860698L (en) Radiation projector producing a highly efficient and highly¹homogeneous flux with controlled apertures angles, in¹particular from a point or quase-point source
US3501626A (en) Radiation condenser devices
US2624234A (en) Projection illumination system for the homogeneous distribution of light
US1928539A (en) Antidazzling headlight