CA2076090A1

CA2076090A1 - Electric lamps having a lens shaped arc or filament chamber

Info

Publication number: CA2076090A1
Application number: CA002076090A
Authority: CA
Inventors: Paul G. Mathews
Original assignee: Individual
Current assignee: General Electric Co
Priority date: 1991-08-29
Filing date: 1992-08-13
Publication date: 1993-03-01
Also published as: JPH05205698A; KR930005508A; EP0534606A1

Abstract

ELECTRIC LAMPS HAVING A LENS SHAPED
ARC OR FILAMENT CHAMBER
ABSTRACT

An electric lamp having either an arc or a filament as the light source enclosed within a light transmissive chamber whose wall is in the shape of a positive or convergent lens. Such lamps increase the amount of light emitted in a direction normal to the filament or arc axis and when mounted in a reflector result in more light being reflected within the desired beam pattern.

Description

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ELECTRIC LAMPS H~VING A LENS SHAPED
ARC OR FILAMæNT caAMBER
BA~R9~ OF TH~ INV~NTION - -This invention relates to electric lamps having an arc or filament chamber whose wall is in the shape of a convergent lens. Mor~ particularly this invention relates to an electric lamp having either an arc or filament as the light source which is cnclo3ed within an arc or filament chamber whose wall is in the shape of a positive or convergent lens for increasing the amount of light emitted in a direction perpendicular to the longitudinal axi~ of the arc or filament and reducing the amount of light e~itted in a direction towards the longitudinal axis of the arc or filament.

Back~round of the Inve~a Arc discharge lamps comprising a vitreous arc tube enclosing electrode~ and an arc sustaining fill within are well known to those in th~ art as are incandescent lamps wherein a tungsten filament is enclosed within a vitreous ~ilament chamber. Such lamps are available in various shapes and sizes with the arc discharge chamber or ~ilament chamber generally being o~ a cylindrical, spherical or elliptical shape. ~xcept for sodium lamps . .
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-~ , which employ a ceramic arc chamber, the arc chamber of discharge lamps and the filament cha~ber of high intensity incandescent lamps ~re formed from a transparent vitreous material capable of withstanding the high temperature generated by the arc with fused silica (quartz) being the material of choice at the present time. Tungsten-halogen lamps are high intensity ~ilament lamps which are most often used mounted within a reflector for various types of lighting applications, including automotive lighting.
Miniature arc discharge lamps are also used within a reflector for automotive and other lighting applications. In lighting applications wherein a lamp is mounted within a reflector, i~ i~ desirable for all or at least most o~ the light emitted by the lamp to strike the reflecting sur~ace and be reflected forward of the reflector in the desired beam pattern, with minimal light distribution outside the beam pattern.

SUMMA~ OF THE INVENTION

The present invention relate~ to an electric lamp having an arc discharge or filament as the light source within an arc or filament chamber, wherein the wall of the arc or filament chamber is in the shape of a positive or convergent lens. This increases the amount Z5 of light emitted by the lamp in a direction normal to the lonyitudinal axis of the lamp and reduces the amount of light emitted in a direction towards the longitudinal axis Or lamp. When lamps of this invention are mounted in a re~lec~or, the positive or convergent len~ shape of the arc or filament chamber wall increases the amount o~ light reflected from the reflecting surface into the desired beam pattern and reduce~ the amount of light outside the de~ired beam pattern. Thi~ i~ a re~ul~ of more o~ the light emitted by the lamp striking the raflecting surface and being 3'3~3 -3- LD 999~

projected fsrward of the reflector within the desired beam pattern. Thus, one embodiment of this invention relates to a reflector and lamp combination whe~in an arc discharge lamp or incandescent lamp is mounted within a reflector wherein the wall of the arc discharge chamber or filament chamber has a positive lens shape. Using a lamp of the present invention in this combination produces more reflected light than would be possible with a conventional arc lamp or filament lamp of the same light emissivity, but wherein the wall of the arc or ~ilament cha~bsr is of a relatively uniform thicknes~.

By convergent or positive lens is meant a lens which converges light. ~xamples of such lenses include a plano-convex lens, a positive meniscus lens and a bi-or double-convex lens. Arc discharge lamps according to this invention have been made with the arc chamber wall having both plano-convex lens shapes and positive meniscus lens shapes. In the context of the lamps of the present invention, positive shape means that the thickness of the arc chamber or filament chamber wall is greater towards the middle than ak ~he ends thereo~. Those skilled in the art will understand that in some embodiments it will be undesirable or impractical for the arc chamber wall to be thickest exactly at ~he mid~le. Thus, in double ended lamps of this invention, a section of the arc or filament cha~ber w~ll taken in a direction parallel to the arc or ~ilament will have a generally plano-convex, double convex or positive meniscus lens shape. In single ended and electrodele~s ~amps, such as those disclosed, for example, in U.S. Patents 4,409,516: 4,620,130:

4,723,092: 4,876,483 and 4,894,590 those skilled in the art will recogniz~ yet other possibilities exist fsr place~ent o~ the positive lens portion of ths arc or filament chamb~r wall.

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-4- ~D 9993 BRIEF DESCRIPTION OF TH~ DRAWINGS

Figure l(a) schematically illustrates a miniature arc lamp of the prior art; Fi~ures l(b), l(c) and l(d) schematically illustrate and miniature arc lamps of the invention, and Figure l(e) schematically illustrates a filament lamp of the invention.

Figure 2 schematically represents an arc lamp of the prior art in 2(a) and an arc lamp of the invention in 2(b), both mounted within a reflector.

Figure 3 is a perspective Yiew of an automotive headlamp employing a miniature arc lamp of th~
invention.

Figure 4 schematically repressnts an experimental apparatus used to obtain the data of Figure 5.

Figure 5 is a graph o~ intensity of lamp light output as a function of emission angle of a lamp of the invention.

DETAILED DESC~IPTION OF THE INVENTION

Turning now to Figure ~, in Figure 1(a) a typical prior art miniature metal halide lamp 10 is schematically illustrated comprising ~used silica e~velope 12 having an in~ernal arc chamber 14 which ~nclose~ a pair of electrod~ 16 and a ~ill including mercury, at least one ~etal halide and inert starting gas (not shown). Arc chamber wall 13 is o~ uni~orm thickne~ and i~ sho~n in a generally elliptical shape, al~hough it could b~ an ovoid ~hap~, a spherical shape, a c~mbination o~ shapes, etc., as i~ well known to those skilled in ~h~ ar~. Electrod~s 16 are .
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hermetically sealed in arc chamber 14 by means of seal portions 18 at each end of the arc chamber which are pinched or shrunk around molybdenum foil seals 20 connected at one end to the electrodes and at the other end to outer leads 22. The two arrows depict light radiation emitted from the midpoint of the arc (not shown) which would be at the midpoint between the two electrode~. One arrow illustrate~ light being emitted in a direction perpendicular or normal to the longitudinal axis of the lamp (and arc) and the other arrow illustrate~ light being emitted at an angle 9 in a direction towards th~ longitudinal axis of the lamp.

Figure l(b) schematically illustrates a miniature double ended metal halide arc lamp 30 of the present invention which also comprises a ~used silica envelope 32 having hermetically sealed arc chamber 34 enclosing electrodes 16 and a suita~le fill hermatically sealed therein by means o~ shrink or pinch seals 18~ Wall 33 of envelope 32 is in the shape of meniscus lens which is a positive or convergen~ type of lens. Seals 18 hermetically seal molybdenum sealing foils 20 connected at one end to electrode~ 16 and at the o~her end to outer leads 22 as with the prior art arc lamp. As with the prior art lamp, one arrow illu~trates ligh~
radiation e~itted by the arc in a direction normal or 90' to She longitudinal axis o~ both the arc and lamp.
Th¢ other arrow illu~trates light emitted at an angle e which is identical to the angle e of the prior art lamp illustra~ed in Figure l(a), but wherein the positive or convergant hape oX the arc chamber wall 33 bends the light radiation emitted by the arc at the e angle in a direction more normal to the longitudinal axis of the arc and lamp as it passes through wall 33.

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This converging or collimating of the light radiation emitted by lamps of the inv~ntion is also shown in Figures l(c), l(d) and l(e). Thu~ in Figure l(c) lamp 40 comprises fused silica envelope 42 wherein the wall 43 of arc chamb~r 44 is in the shape of a plano-convex lens. In Figure l(d) lamp 50 is shown comprising fused silica envelope 52 wherein wall 53 of arc chamber 54 is in the shape of a double convex lens. In bo~h of these embodiments the light emitted by the arc at the e angle i5 bent in a direction more normal to the longitudinal axis of the lamp and arc by the convergent len~ shape of the arc chamber wall. Figure l(e) schematlcally illustrates another embodiment o~ a lamp of the invention wherein the source of light is a tungsten filament 65 enclosed within filament cha~ber ~4 wherein chamber wall 63 is in the shape of meniscus lens such as is shown in Figure l(b). In this latter embodiment a shorter filament (as shown) is preferred over a long filament, because the lensing eff~ct is more effective for a shorter light source than for a longer light source whether such source be an arc or a filament. The ideal light source for maximum lensing e~fect is a poin~, but this doesn't exist in practicality. For example, if the filament chamber is elliptical, the length of the filament will preferably be shorter than the distance between the two focal points of the ellipse. Also, the lamp may be a conventional incandescent lamp or i~ may be a tungsten-halogen lamp wherein one or more halogen compounds are enclosed within the filament cha~ber as i~ well known to those skilled in the art. In a ~urther embodiment ~ha outer sur~ace of the filament chamber may be coated with a multi-layer light interference ~oating made o~ alt~rnating layers of high and low refractive index materials such as tantala and silica.

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-7-- I.D 9993 Double ended lamps according to this invention have been made with both plano-convex lens shapes and positive meniscus lens shapes by means of a process employing a gathering-molding process disclosed in column ~ of U.S. Patent 4,810,932, in column 9 of 4,389,201 and in a paper by Hansler and Davenport, "A
New Low Wattage Metal Halide Lamp Process", J. IES, p.
109-122 (Fall, 1985), the disclosures of which are incorporated herein by reference. Thess references disclose gathering-molding process which may be employed to make lamps out of high temperature glass or fused silica or synthstic quartz. This gathering and blow molding process is performed on a glass lathe which is controlled by a computer to ensure conformance to the specifications that have been s~t for the inside and outside surface profiles of the arc or filament chamber. In such a process a hollow cylindrical piece of synthetic quartz or fused silica tubing is loaded into a glass lathe with a seal made to both ends of the tubing to ensure that a positive gas pressure can be applied inside the tubing during rotation, heating and molding o~ the tubing. As the lathe collet rotates, a gas torch is direct~d toward that portion of the tubing at which it is desired to form the arc or filament chamber. The ~orch is designed to heat only a short length o~ the tubing and it is dxiven along the length of the tubing while one end of the tubing is slowly pushed towards the other end which is fixed in the collet. This cause~ the ~uartz thickness to be increased where the torch flame is directed. A
combination of positive pressure inside the tubing and the lower viscosity at the inside surface of the tubing due to the lower in~ide surface ~emperature maintains or minimizes the collapse o~ the interior of the tubing during tha forming process. In thi~ man~er the quartz wall thicXness can b~ built up ~rom about 1 mm thick to several ~m thick when employing, for exampla, quartz ' , .

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tubing typically 3 x 5 x 150 or similar (ID x OD x length in mm). When the desired gather has been achieved the torch s shut off and moved out of th~
work area. Also, during this process it is advantageous to have a cooler gas stream located at either side of the torch flame in order to maintain that portion of the chamber/tubing cool adjacent the hot portion while the gathering is occurring in the area being heated by the flame. After the gather process is compl~te a molding torch typically longer than the arc or filament chamber and wider than the tubing is employed to heat the entire chamber and when the proper temperature i5 reached a mold is indexed into position over the cha~ber and enclosed around the chamber. A positive pressure is then applied, via head and tail stock seal~, to the inside of the chamber forcing the hot quartz to expand to the inside shape o~
the mold. After the molding is complete the mold and torch are removed from the work area and the fully molded tube is ready for finishing.

Turning to Figure 2, both a prior art lamp 10 and a lamp 30 of the pr~sent invention are shown having an elongated stem portion 19 forming one end of the vitreous lamp envelope mounted (by mean~ not shown) into a base portion 74 of a reflector 70 having light reflecting surface 72 on the in~ide thereof. Conductor 71 is electrically connected to lamp outer l~ad 22, ex~nds ~hrough hole 7~ in re~lectur 70 and is connected to a ground (not shown~. Similarly, high voltage insulated conductor 75 is connected by means not shown to ths other ou~er lead of lamp 10 and lamp 30 and exits base 74 from which it is conn~cted to a high voltage current supply which is not shown. In opera~ion, visible light radia~ion, a, emitted by the arc ~ube in a direction normal to the longitudinal axis o~ the lamp strik~s ~he re~lectlve sur~ace of the g~

-9- LD g593 reflector and is reflected and projected forward in the desired beam pattern. With the prior art lamp 10, visible light radiation de~icted as b ~nd c emitted from the center of the arc chamber off normal to the S longitudinal lamp axis at angles ~1 and ~2~
respectively, continue in the ~1 and ~2 directions and are not reflected forwardly off reflective surface 72.
Instead, visible light radiation b and c miss the reflective surface 72 and exit in a direction more to the side of the reflector instead of being projected forward of the reflector in the desired beam pattern as with light radiation, a. In con~ras~, employing a lamp 30 of the present invention wherein the arc chamber wall is in the form of a positive lens results in the light radiation emitted from the center of the arc at angles ~1 and ~2 to be convergently refracted by the positive lens shape of the arc chamber wall so that they exit the arc chamber at angles ~3 and ~4 which are smaller than ~1 and ~2. As a conseguence, the light radiation b and c in this embodiment emitted at angles ~3 and 74, respectively, strike the reflecting surface 72 of the reflec~or as part of the desired beam pattern. Thus, by using a lamp having an arc or filament chamber wall in the shape of a convergent or positive lens, a greater amount of light emitted by the lamp is reflected from the reflecting surface and projected forward of the reflector within the desired bea~ pattern and not lost a radiation ~mitted outside the desired beam pattern.

~urning to Figure 3 another embodiment of the present invention is illustrated wherein lamp 30 (Figure l(b)) is mounted horizontally within an automotiv2 headlamp assa~bly 80 comprising a double truncated, parabolic reflecting member 82 with a lens 84 secured to the ~ront section of the reflector member, a connection mean~ 86 secured at the rear 2 ~

section of the reflector member for conneotion to a power source and arc lamp 30 mounted within. Lamp 30 is mounted within reflec~or 82 by means of electrically conductive metal support leads 96 and 97 which are welded at one end ~o lamp leads 22 and connected at their other end to pins 98 for connection to a source of electricity. Lamp 30 is mounted vertically in reflector 82 with its longitudinal axis normal to longitudinal axis 88 of the re~lector and top and bottom flat truncated portions 90 and 92, while being gener~lly parallel to parabolic reflecting portion 94.
Thus, the positive cxoss section of the arc chamb~r wall increases the amount o~ emitted light directed to the parabolic reflecting surface. The interior surface (not shown) o~ the parabolic reflecting portion g4 is a light reflecting surfac~ ~or reflecting light emitted by lamp 30 ~orward of the reflector in a predetermined beam pattern. Mounting lamp 30 of the invention in the reflector 82 in the fashion shown and described increases the lamp light output that is reflected forward of the reflector, while at the same time reducing the amount of light emitted by the lamp in a direction that will strike the truncated portions 90 and 92 of the re~lector, which light is not projected forward into the desired beam pattern and is thereby wasted.

The foregoing embodiments are meant to be illustrative and not limiting examples of the practice of the invention. Thu~ aro lamps use~ul in the practice o~ the inv~ntion ar~ not limited to those containing metal hali~e, but include mercury, xenon, etc., arc lamps. Further, the invention may also ~e practiced with ~ingle ended arc and f ilament lamps and al~o with electrodele~s la~p~ a~ di~cussed under Summary of the Invention. In ~he cas~ o a Qingle ended lamp comprising an arc or filament chamb~r having , , ~

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~ LD 9993 a top, sides and bottom, wherein the leads connect~d to the filament or electrode extend through a hermetic seal in the bottom, all or a portion of the top and/or side walls of the chamber could be in the form of a positive lens shape as could all or a portion of the wall(s) of an electrodeless lamp arc chamber. Further, even with the double ended examples illustrated and described above, not all o~ the arc chamber wall need be in the shape of a convergent lens.

Figure 4 schematically illustrates an experimental arrangement used to mea~ure the degree of lensing or light collimation that occurr~d in arc lamps of the inven~ion having w211s in the shap~ of a positive or convergent m~niscus lens, such as is shown in Figure l(b), compared to si~ilar types of prior art lamps such as is shown Figure 2(a) wherein the wall of the arc chamber had a relatively uniform cross section. Each arc tube or lamp to be measured was mounted on a rotary table (not shown), wi~h the midpoint of the arc chamb~r 50 centimeters from a light detecting photodidode 100, which in turn wa electrically connected to a volt meter 102. Each ar~ tube to be measured was mounted on a rotary table (not shown) with its longitudinal axis horizontal. The rotational axis of the table was coincident with the middle of the aro cha~ber of the arc tube. The light detecting photodiode or photocell, corrected fox human eye sensitivity, was a United Detector Technology PINlOhP. The active ar~a of the photocell was directed toward the center of the lamp arc chamber The voltage measured across the photodiode was proportional to the amount of light striking it. This configuration permittPd rotation of the arc tube while it was energized in order to vary th~ v$ewing angle of the arc t~be by th~ photodiode detector and maintain the distanc~ ~rom ~h~ cent~r of the arc chamb~r ~o the detec~or constant. Thu~ the "S~J~J~

amount of light directed toward the detector from ~he lamp could be determined as a function of various viewing angles. Metal halide lamp arc tubes representative of the prior art had an electrode gap 5 mm long hermetically enclosed, along with metal halide and mercury and an inert starting gas, in a 9 x 7 mm ellipsoidal arc chamber. The arc chamber wall was of uniform thickness and was 0.6 mm thick. These lamps were made from a 2.4 x 4 mm fused silica or quartz stock. Lamps according to the present invention had a similar fill with an electrode gap o~ 4.2 mm in an ellipsoidal arc cha~ber having dimensions 9 x 6.7 mm with a 2.7 mm inside diameter and a meniscus lensing wall cross section of the arc chamber. These lamps were made from tubing stock having a dimension of 1.8 x 3.2 mm. In both of these lamps the 7 mm or 6.7 mm dimension was the maximum out~ide diameter of the arc chamber. The given dimensions o~ the tubing stock from which the lamp was made are the inside and outside diameters, respectively, of the tubing. The thickness of the arc chamber wall of the lamps of the present invention was 2.0 mm at its thickest point in the middle of the arc chamber and gradually reduced to about 1.3 mm at each end of the arc chamber.

Figure 5 graphically displays intensity o~ light output as a function o~ emission angle of lamps of the -present invention and lamps of the prior art th~t were measured using the apparatus schematically shown in Figure 4. The results shown in Figure 5 dramatically illustrate the invention in that the lamps of the present invention having an arc chamber whos~ wall is in the shape of a positive or conver~ent lens significantly collimates the light emitted from the arc cha~ber so ~hat mor0 of the light is e~itted in a direction perpendicular to the longitudinal axis of the arc. All o~ the curve~ in Figure 5 were normalized to .

-13~ LD 9993 the peak intensity of each lamp, because the different designs produced different lumens. The relative light intensity was determined by dividing the light intensity exhibited at each viewing angle by the maximum intensity observed and this is plotted in Figure 5 as a function of viewing angle. The relatively flat intensity profile exhibited by the lamps of the prior art indicates a lack of any lensing effects. The abrupt drop in intensity at the 90-viewing angle was due to the light being blocked by theseal at the end of the lamp in an end-on view by the photodiode detector. The curves of the lamps of th~
invention show that the amount of light radiated by the lamps at large angles relative to the non-lensing prior art lamps were substa~tially reduced.

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Claims

1. An electric lamp having a light transmissive arc or filament chamber enclosing an arc or filament as the light source within, wherein said chamber has at least one wall at least a portion of which is in the shape of a positive or convergent lens.

2. The lamp of claim l wherein at least a portion of light emitted by said lamp is refracted by said wall lens.

3. The lamp of claim 2 wherein said positive lens shape is a meniscus lens, a plano-convex lens or a double-convex lens.

4. The lamp of claim 3 wherein the maximum thickness of said lens-shaped chamber wall is greater towards the middle of said chamber than at the end.

5. The lamp of claim 3 being an electrodeless arc lamp.

6. The lamp of claim 3 being an arc discharge lamp having said arc chamber enclosing a pair of electrodes within.

7. The lamp of claim 3 being an incandescent lamp wherein said filament chamber encloses a filament within.

8. An electric arc lamp having a pair of electrodes and a suitable fill hermetically enclosed within a light transmissive arc chamber, wherein at least a portion of the wall of said chamber is in the shape of a convergent lens and wherein at least a portion of light emitted by said arc is refracted by said lens shaped arc chamber wall.

9. The lamp of claim 8 being a double-ended lamp with one of each of said electrodes being located at a respective end of said chamber.

10. The lamp of claim 9 wherein the maximum thickness of said lens shaped chamber wall is greatest towards the middle of said chamber than at the ends thereof.

11. The lamp of claim 10 wherein at least a portion of said refracted light is emitted in a direction more towards normal to the arc axis.

12. An electric incandescent lamp having a light transmissive filament chamber having a filament hermetically enclosed within wherein at least a portion of the wall of said chamber is in the shape of a convergent lens and wherein at least a portion of light emitted by said filament is refracted by said lens shaped portion of said wall.

13. The lamp of claim 12 being a double ended lamp and said chamber and filament each having a longitudinal axis parallel to each other.

14. The lamp of claim 13 wherein the maximum thickness of said lens shaped chamber wall is greatest towards the middle of said chamber than at the ends thereof.

15. The lamp of claim 14 wherein at least a portion of said refracted light is emitted in a direction more towards normal to the arc axis.

16. In combination, a reflector and an electric lamp mounted within said reflector, said lamp having an arc or filament chamber enclosing an arc or filament as the light source within, wherein said chamber has at least one wall at least a portion of which is in the shape of a positive or convergent lens and wherein at least a portion of light emitted by said source is refracted by said lens shaped portion of said wall.

17. In combination, a reflector and a double ended electric lamp mounted within said reflector, said lamp having an arc or filament chamber enclosing an arc or filament as the light source within, wherein said chamber wall is in the shape of a positive or convergent lens and wherein at least a portion of light emitted by said source is refracted by said lens shaped wall.

18. The invention as defined in any of the preceding claims including any further features of novelty disclosed.