WO1994022160A1 - Light plus - Google Patents
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- Publication number
- WO1994022160A1 WO1994022160A1 PCT/US1993/002760 US9302760W WO9422160A1 WO 1994022160 A1 WO1994022160 A1 WO 1994022160A1 US 9302760 W US9302760 W US 9302760W WO 9422160 A1 WO9422160 A1 WO 9422160A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- light
- tube
- reflective layer
- centre
- reoriented
- Prior art date
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21V—FUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
- F21V17/00—Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages
- F21V17/04—Fastening of component parts of lighting devices, e.g. shades, globes, refractors, reflectors, filters, screens, grids or protective cages the fastening being onto or by the light source
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J61/00—Gas-discharge or vapour-discharge lamps
- H01J61/02—Details
- H01J61/025—Associated optical elements
Definitions
- the present invention reorients the light flux of a fluorescent tube to places where it is needed most yielding a larger intensity of visible light. More specifically, it reorients a maximum quantity of light flux with the greatest efficiency in the direction desired.
- the method proposed here attempts to minimise the losses due to absorption, remission, and reflection caused whenever light strikes a surface by minimising the number of reflections light undergoes before reaching the areas where it is most needed.
- This reflective layer is that of the cylindrical light tube with which it functions.
- This reflective layer corresponds to the same centre of the cylindrical light tube with which it functions.
- the reflective layer is mounted on the surface either inside or outside the cylindrical light tube with which it functions.
- fluorescent tube One important type of cylindrical light tube for which the invention can be applied is the fluorescent tube.
- the operation of such light tubes is well known. Briefly, an electric discharge across a low pressure mercury vapour produces emissions of ultraviolet light at a
- SUBSTITUTE SHEET frequency of 2537A Although light at this frequency is not visible to humans, this light impinges a thin fluorescent layer coating the inside of the light tube to produce visible light according to Stokes Law. The resulting light contains a part perpendicular to the surface of the tube.
- the primary light emitted normally to the surface of the tube is reoriented in the opposite direction, passes through the centre and exits from the other side of the tube toward the areas desired.
- the secondary light emitted at other angles to the surface of the tube is reoriented near the centre of the tube or again toward the mirror and follows a path to exit from the other side of the tube toward the desired areas (see Figures 3a and 3b).
- the system is mounted outside the tube and directly reorients the visible light produced by the fluorescent layer of the tube.
- the second way consists of mounting the system inside the tube to reorient the ultraviolet rays toward the other side of the tube where they undergo the process of fluorescence and consequently produce visible light.
- the results are the same: the visible light flux composed of reoriented light and non-reoriented light, is more intense in the directions where it is most desired.
- the invention is implemented by a system composed of an extremely reflective layer that is in direct contact with the surface of the tube, either on the interior or exterior surface of the tube.
- the simplest system consists of two parts:
- the thin reflective layer serves as the mirrored surface of the system. It is from a flexible material like plastic or paint with high reflectivity (greater than 95% reflectivity) and resistant to the average operational temperature of a standard fluorescent tube. The size of this thin layer depends on the tube with which it functions as well as the quantity of light flux desired (see Section Results).
- the mechanism of attachment serves to put in contact the thin reflective layer with the fluorescent tube. It is accomplished with a cohesive material like tape or clips as shown in Figures la and lb.
- the cohesive material or clips are made of non-toxic materials which are resistant to the average operational temperature of a standard fluorescent tube.
- the adhesive material or clips are placed at each extremity of the thin reflective layer as well as at regular intervals along the length of the tube.
- Two versions of the invention have been created and tested, notably one with tape and one using clips.
- the two versions covered 50% of the surface of the light tube by the reflective layer and functioned outside the light tube. It should be mentioned that the workings of the system are exactly the same for application of the invention inside the tube, except for the fact that it is necessary to change the reflective material to that for ultraviolet light.
- the invention increased the light flux between 32% and 36% to the areas desired,
- the invention In comparison to a fluorescent tube with its original system of light diffusion, the invention increased the light flux between 11% a and 23% to the areas desired (according to the original system of diffusion), corresponding to an efficiency of reorientation between
- the quantity of light flux which can be attained corresponds exactly to the surface of the fluorescent tube covered divided by the area of the surface of the entire tube according to the inverse square law for the flux of light. In application, this quantity corresponds to the angle swept by the circular-reflective layer covering the tube.
- the corresponding quantity of light flux which can be attained by the system is calculated from the following formula:
- SUBSTITUTE SHEET the direction of the reoriented light flux can be controlled by this method through the orientation of the thin layer on the light tube.
- the present invention proposes a method of reorientation of light flux with a circular mirror system having the same form, the same radius, and the same centre as that of the light tube with which it functions. This allows each normal ray of light to be reoriented in the opposite direction toward the centre of the light tube.
- the reoriented light flux passes from the centre of the light tube, exits the tube at the other side, and combines with the non- reoriented light flux to result in more visible light.
- a cohesive material or clips connect the thin layer of extremely reflective material to the surface of the tube.
- the system functions outside the tube by directly reorienting the visible light or inside the tube by reorienting the ultraviolet light that then undergoes the phenomena of fluorescence on the other side of the tube.
- the invention has several advantages for increasing the visible light flux to areas desired. Among these advantages are the following:
- TUTE SHEET 4 The system costs less than the average price of a standard fluorescent tube.
Landscapes
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- Vessels And Coating Films For Discharge Lamps (AREA)
Abstract
A method of light reorientation and recovery, is based on circular mirror system (figure 2) that has the same radius of curvature and the same center as that of the light source with which the system functions. These characteristics allow the system to reorient light rays striking the surface normally in the opposite direction toward the centre of the light source. This reoriented light flux passes through the centre of the light tube, exits, and combines with the non reoriented light flux to give more visible light to the areas desired. In a fluorescent tube, the system is mounted outside the light tube surface, and directly reorients the visible light, or mounted inside the light tube surface, and reorients the ultraviolet light toward the other side of the tube where it then undergoes fluorescence. In either case, the end result is more visible light to the areas where it is desired.
Description
Description: Light Plus
Introduction :
The present invention reorients the light flux of a fluorescent tube to places where it is needed most yielding a larger intensity of visible light. More specifically, it reorients a maximum quantity of light flux with the greatest efficiency in the direction desired. The method proposed here attempts to minimise the losses due to absorption, remission, and reflection caused whenever light strikes a surface by minimising the number of reflections light undergoes before reaching the areas where it is most needed.
Theory of the Invention:
The invention is based on a method of reflecting light rays by a system characterised by the following:
- A thin reflective layer which is circular in form.
- The radius of curvature of this reflective layer is that of the cylindrical light tube with which it functions.
- The centre of this reflective layer corresponds to the same centre of the cylindrical light tube with which it functions.
- The reflective layer is mounted on the surface either inside or outside the cylindrical light tube with which it functions.
These characteristics allow the system to reorient each light ray striking its surface normally in the opposite direction toward the centre of the cylindrical light tube (see Figures 2a, 2b, 3a, and 3b). The reoriented light flux passes through the centre of the tube, exits the tube on the opposite side, and combines with the non-reoriented light rays resulting in a greater intensity of the visible light.
Application to the Fluorescent Tube:
One important type of cylindrical light tube for which the invention can be applied is the fluorescent tube. The operation of such light tubes is well known. Briefly, an electric discharge across a low pressure mercury vapour produces emissions of ultraviolet light at a
SUBSTITUTE SHEET
frequency of 2537A. Although light at this frequency is not visible to humans, this light impinges a thin fluorescent layer coating the inside of the light tube to produce visible light according to Stokes Law. The resulting light contains a part perpendicular to the surface of the tube.
This is the reason this method of reorientation applied to the fluorescent tube is characterised in the following ways:
- The primary light emitted normally to the surface of the tube is reoriented in the opposite direction, passes through the centre and exits from the other side of the tube toward the areas desired.
- The secondary light emitted at other angles to the surface of the tube is reoriented near the centre of the tube or again toward the mirror and follows a path to exit from the other side of the tube toward the desired areas (see Figures 3a and 3b).
This is also the reason that the application of the method to the fluorescent tube is distinguished in two different ways. In the first, the system is mounted outside the tube and directly reorients the visible light produced by the fluorescent layer of the tube. The second way consists of mounting the system inside the tube to reorient the ultraviolet rays toward the other side of the tube where they undergo the process of fluorescence and consequently produce visible light. Regardless of the way the method is applied to the fluorescent tube, the results are the same: the visible light flux composed of reoriented light and non-reoriented light, is more intense in the directions where it is most desired.
Model:
In practice, the invention is implemented by a system composed of an extremely reflective layer that is in direct contact with the surface of the tube, either on the interior or exterior surface of the tube. The simplest system consists of two parts:
1) A thin reflective layer.
2) A means of attachment to the tube.
TE SHEET
The layout of the system is shown in Figures la and lb.
1) The Thin Reflective Layer
The thin reflective layer serves as the mirrored surface of the system. It is from a flexible material like plastic or paint with high reflectivity (greater than 95% reflectivity) and resistant to the average operational temperature of a standard fluorescent tube. The size of this thin layer depends on the tube with which it functions as well as the quantity of light flux desired (see Section Results).
2) The Means of Attachment
The mechanism of attachment serves to put in contact the thin reflective layer with the fluorescent tube. It is accomplished with a cohesive material like tape or clips as shown in Figures la and lb. The cohesive material or clips are made of non-toxic materials which are resistant to the average operational temperature of a standard fluorescent tube. The adhesive material or clips are placed at each extremity of the thin reflective layer as well as at regular intervals along the length of the tube.
Two versions of the invention have been created and tested, notably one with tape and one using clips. The two versions covered 50% of the surface of the light tube by the reflective layer and functioned outside the light tube. It should be mentioned that the workings of the system are exactly the same for application of the invention inside the tube, except for the fact that it is necessary to change the reflective material to that for ultraviolet light.
Results :
Two different types of tests have been performed for the two models of the invention: 1) A test with an isolated fluorescent tube and 2) A test with the fluorescent tube and its original system of light diffusion.
1 ) In comparison to the isolated fluorescent tube, the invention increased the light flux between 32% and 36% to the areas desired,
SUBSTITUTE SH---EF
corresponding to an efficiency of reorientation between 64% and
72%.
2) In comparison to a fluorescent tube with its original system of light diffusion, the invention increased the light flux between 11% a and 23% to the areas desired (according to the original system of diffusion), corresponding to an efficiency of reorientation between
22% and 46%.
Theoretically, the quantity of light flux which can be attained corresponds exactly to the surface of the fluorescent tube covered divided by the area of the surface of the entire tube according to the inverse square law for the flux of light. In application, this quantity corresponds to the angle swept by the circular-reflective layer covering the tube. The corresponding quantity of light flux which can be attained by the system is calculated from the following formula:
where Fideaι represents the ideal quantity of light flux added in per cent, C represents the angle swept by the circular-reflective layer of the system covering the tube in radians, and 1κ is the angle traversed by a circle in radians. Actually, this formula represents the ideal case, however in practice the efficiency of the reflection must be taken into account as shown in the following formula:
where Freai is the real quantity of light flux increased in per cent and £ represents the efficiency of reorientation. This is the reason why the method of reorientation of the light flux is characterised by the angle swept by the reflective layer and corresponds to the quantity of light flux obtained up to 50%. This is also the reason that
SUBSTITUTE SHEET
the direction of the reoriented light flux can be controlled by this method through the orientation of the thin layer on the light tube.
Although it is possible to cover more than 50% of the surface of the light tube, the results are less efficient. In fact, the most efficient results are obtained when 50% of the surface of the tube is covered by the thin layer and 50% is exposed to the areas desired (see Figures 2a and 2b). Under these conditions, 50% of the light exits directly from the fluorescent tube and the other 50% after reflecting from the reflective layer a minimum number of times.
Conclusion :
In conclusion, the present invention proposes a method of reorientation of light flux with a circular mirror system having the same form, the same radius, and the same centre as that of the light tube with which it functions. This allows each normal ray of light to be reoriented in the opposite direction toward the centre of the light tube. The reoriented light flux passes from the centre of the light tube, exits the tube at the other side, and combines with the non- reoriented light flux to result in more visible light.
In application of the invention to the fluorescent light tube, a cohesive material or clips connect the thin layer of extremely reflective material to the surface of the tube. The system functions outside the tube by directly reorienting the visible light or inside the tube by reorienting the ultraviolet light that then undergoes the phenomena of fluorescence on the other side of the tube.
In application to the fluorescent tube, the invention has several advantages for increasing the visible light flux to areas desired. Among these advantages are the following:
1) The system doesn't use electricity.
2) The system possesses a life which is practically unlimited.
3) The system installs directly on the lighting which is in place and in the same time as that for a simple fluorescent tube.
TUTE SHEET
4) The system costs less than the average price of a standard fluorescent tube.
5) The system increases the visible light flux up to 36% to the areas desired.
SUBSTITUTE SHEET
Claims
1. The method of reorientation of light flux otherwise disperses away from the desired areas for cylindrical light tubes. The method is characterised by the fact that:
- The primary light emitted normally to the surface of the tube is reoriented in the opposite direction, passes through the centre, and exits from the other side of the tube toward the areas desired.
- The secondary light emitted at other angles to the surface of the tube is reoriented near the centre of the tube or toward the reflective surface and follows a path to exit the tube toward the desired areas.
2. The method in accordance with Claim 1 and effectuated by a reflective system which is characterised by the following:
- A thin reflective layer which is circular in form.
- The radius of curvature of this reflective layer is that of the cylindrical light tube with which it functions.
- The centre of this reflective layer corresponds to the same centre of the cylindrical light tube with which it functions.
- The reflective layer is mounted on the surface either inside or outside the cylindrical light tube with which it functions.
3. The method according to Claims 1 and 2 and characterised by the fact that the angle swept out by the reflective layer on the cylindrical light tube is directly related to the quantity of light flux obtainable and for which the direction can be controlled by the orientation of the reflective layer on the light tube.
SUBSTITUTE SHEET
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/US1993/002760 WO1994022160A1 (en) | 1993-03-22 | 1993-03-22 | Light plus |
AU39672/93A AU3967293A (en) | 1993-03-22 | 1993-03-22 | Light plus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/US1993/002760 WO1994022160A1 (en) | 1993-03-22 | 1993-03-22 | Light plus |
Publications (1)
Publication Number | Publication Date |
---|---|
WO1994022160A1 true WO1994022160A1 (en) | 1994-09-29 |
Family
ID=22236444
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/US1993/002760 WO1994022160A1 (en) | 1993-03-22 | 1993-03-22 | Light plus |
Country Status (2)
Country | Link |
---|---|
AU (1) | AU3967293A (en) |
WO (1) | WO1994022160A1 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1999060303A1 (en) * | 1998-05-18 | 1999-11-25 | Minnesota Mining And Manufacturing Company | Light reflective film and light emitting apparatus |
WO2002048606A2 (en) | 2000-12-11 | 2002-06-20 | 3M Innovative Properties Company | Luminaire comprising an elongate light source and a back reflector |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3225241A (en) * | 1959-07-09 | 1965-12-21 | Sylvania Electric Prod | Aperture fluorescent lamp |
US3767956A (en) * | 1969-12-24 | 1973-10-23 | Xerox Corp | Aperture fluorescent lamp for copying machines |
US4255687A (en) * | 1978-02-10 | 1981-03-10 | U.S. Philips Corporation | Low pressure mercury vapor discharge lamp |
US4336479A (en) * | 1978-11-08 | 1982-06-22 | Hitachi, Ltd. | Fluorescent lamp having reflective layer and a method for fabricating the same |
-
1993
- 1993-03-22 WO PCT/US1993/002760 patent/WO1994022160A1/en active Application Filing
- 1993-03-22 AU AU39672/93A patent/AU3967293A/en not_active Abandoned
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3225241A (en) * | 1959-07-09 | 1965-12-21 | Sylvania Electric Prod | Aperture fluorescent lamp |
US3767956A (en) * | 1969-12-24 | 1973-10-23 | Xerox Corp | Aperture fluorescent lamp for copying machines |
US4255687A (en) * | 1978-02-10 | 1981-03-10 | U.S. Philips Corporation | Low pressure mercury vapor discharge lamp |
US4336479A (en) * | 1978-11-08 | 1982-06-22 | Hitachi, Ltd. | Fluorescent lamp having reflective layer and a method for fabricating the same |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1999060303A1 (en) * | 1998-05-18 | 1999-11-25 | Minnesota Mining And Manufacturing Company | Light reflective film and light emitting apparatus |
WO2002048606A2 (en) | 2000-12-11 | 2002-06-20 | 3M Innovative Properties Company | Luminaire comprising an elongate light source and a back reflector |
Also Published As
Publication number | Publication date |
---|---|
AU3967293A (en) | 1994-10-11 |
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