US20010055098A1 - Light pipe for a projector system - Google Patents
Light pipe for a projector system Download PDFInfo
- Publication number
- US20010055098A1 US20010055098A1 US09/858,514 US85851401A US2001055098A1 US 20010055098 A1 US20010055098 A1 US 20010055098A1 US 85851401 A US85851401 A US 85851401A US 2001055098 A1 US2001055098 A1 US 2001055098A1
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- United States
- Prior art keywords
- light
- light pipe
- pipe
- entrance pupil
- exit pupil
- 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.)
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/14—Details
- G03B21/20—Lamp housings
- G03B21/2006—Lamp housings characterised by the light source
- G03B21/2026—Gas discharge type light sources, e.g. arcs
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S385/00—Optical waveguides
- Y10S385/901—Illuminating or display apparatus
Definitions
- the present invention relates to a light pipe, and more particularly, to a hollow tapering light pipe.
- FIG. 1 is a schematic diagram of a prior art light pipe 10 for a projector system 12 .
- the projector system 12 comprises a light source 14 to generate light 11 and to guide the light 11 to the light pipe 10 , and an image device 16 to project the light gathered by the light pipe 10 to a screen 13 so as to form an image.
- the light pipe 10 is a hollow rectangular pipe set between the light source 14 and the image device 16 to gather and guide the light 11 .
- the light pipe 10 comprises an entrance pupil 18 and an exit pupil 19 .
- the entrance pupil 18 is used to gather the light 11 generated by the light source 14 .
- the light 11 is guided to the image device 16 through the exit pupil 19 .
- FIG. 2 is a position distribution of the light incident upon the entrance pupil 18 in FIG. 1.
- the transverse axis is a distance in the plane 15 in FIG. 1 from the center of the entrance pupil 18 .
- the longitudinal axis is the light intensity. As shown in FIG. 2, the light closer to the center of the entrance pupil 18 is stronger, and the light farther from the center of the entrance pupil 18 is weaker.
- the light pipe 10 does not gather all of the light 11 .
- the light 24 closer to the center of the entrance pupil 18 enters the light pipe while the light 25 farther from the center of the entrance pupil 18 fails to be gathered by the light pipe 10 .
- FIG. 3 is the incident angle distribution of the light incident upon the entrance pupil 18 .
- the transverse axis of FIG. 3 is the incident angle of the light on the plane 15 , and the longitudinal axis is the light intensity.
- the incident angle of a traditional light bulb is in the range of 18-20 degrees.
- the light pipe 10 is a rectangular pipe with homogeneous cross-sections, the angle of the light leaving of the exit pupil 19 is also in the range of 18-20 degrees.
- the optic device for the image device 16 such as the liquid crystal display (LCD) or the digital microscope device (DMD), has an incident angle limitation. Owing to the incident angle limitation, the angle of the light leaving the exit pupil 19 cannot be too large. Usually, light with an angle over 30 degrees cannot be modulated by the liquid crystal display.
- FIG. 4 is a schematic diagram of another prior art light pipe 20 for the projector system 12 in FIG. 1.
- the light pipe 20 differing from the light pipe 10 , has a tapered body.
- the exit pupil 23 of the light pipe 20 is larger than the entrance pupil 22 to reduce the incident angle of the light.
- the light pipes 10 , 20 are designed to reduce the light 25 leaking from the light pipes 10 , 20 while maintaining a small light angle.
- the light gathering efficiency is improved, and the light intensity is increased.
- the prior art light pipes 10 , 20 have the entrance pupil 18 , 22 smaller than or equal to the exit pupil 19 , 23 , the light 25 leaking from the light pipe 10 , 20 is usually quite strong without increasing the volumes of the light pipes 10 , 20 .
- an arc lamp with a longer arc length can be used as the light source to reduce the incident angle in FIG. 3, it also makes the position distribution of the light in FIG. 2 smoother. Then the light leaking from the light pipe 10 , 20 increases, degrading the light gathering efficiency.
- FIG. 2 is the position distribution of the light incident upon the entrance pupil in FIG. 1.
- FIG. 4 is the schematic diagram of another prior art light pipe used in the projector system in FIG. 1.
- FIG. 6 is a view of the light pipe in FIG. 5.
- FIG. 8 is the incident angle distribution of the light incident upon the entrance pupil in FIG. 5.
- FIG. 9 is the angle distribution of the light leaving the light pipe in FIG. 5.
- FIG. 10 is the relation between the opening ratio and the intensity of the light leaving the light pipe in FIG. 5.
- FIG. 11 is the schematic diagram of the light gathering efficiency improvement of the light pipe in FIG. 5 in comparison with the light pipe in FIG. 1.
- FIG. 5 is the schematic diagram of a light pipe 40 of the present invention used in a projector system 42 .
- the projector system 42 comprises a light source 44 to generate light 46 and to guide the light 46 to the light pipe 40 , and an image device 48 to produce an image by projecting the light 46 gathered by the light pipe 40 to a screen 64 .
- the light pipe 40 is set between the light source 44 and the image device 48 , and the projector system 42 is a projector or a liquid crystal display (LCD).
- LCD liquid crystal display
- the light source 44 comprises an arc lamp 54 to generate light 46 , and a light collector 56 , which is a lampshade in the shape of a half ellipsoid, to collect the light 46 generated by the arc lamp 54 and guide the light 46 to the light pipe 40 .
- the arc lamp 54 is a hyper pressure mercury arc light with a long arc length 55 (Ushio, 150W, NSH150), the arc length 55 being around 1.8 mm (0.0709 inches).
- the image device 48 comprises a display panel 58 set on an image path 61 , a plurality of optic lenses 60 A, 60 B and 60 C set between the light pipe 40 and the display panel 58 , and a projection lens 62 .
- the lenses 60 A, 60 B and 60 C are used to guide the light 46 collected by the light pipe 40 to the display panel 58 to form the image.
- the projection lens 62 is set between the display panel 58 and the screen 64 to project the image to the screen 64 .
- FIG. 6 is a perspective view of the light pipe 40 in FIG. 5.
- the light pipe 40 is a hollow, tapering pipe constructed with four trapezoidal flat plates 62 .
- Each of the trapezoidal flat plates 62 comprises a top end 62 A, a bottom end 62 B, and two sides 62 C.
- the sides 62 C of the trapezoidal flat plates 62 are joined together to from the light pipe 40 .
- the light pipe 40 further comprises four reflector walls (mirror coatings) 49 respectively set on the inner surfaces of the four trapezoidal flat plates 62 to reflect the light 46 to the image device 48 .
- the reflector walls 49 absorb the infrared light in the light 46 and reflect the visible portion of the light 46 .
- the light pipe 40 comprises an entrance pupil 50 and an exit pupil 52 .
- the entrance pupil 50 at one end of the light pipe 40 is a rectangular opening formed by the four bottom ends 62 B of the four trapezoidal flat plates 62 .
- the exit pupil 52 at another end of the light pipe 40 is a rectangular opening formed by the four top ends 62 A of the four trapezoidal flat plates 62 .
- the light 46 generated by the light source 44 is guided to the light pipe 40 through the entrance pupil 50 , and the light 46 gathered by the light pipe 40 is guided to the image device 48 through the exit pupil 52 .
- the area of the exit pupil 52 of the light pipe 40 is smaller than the area of the entrance pupil 50 , and the opening shape of the exit pupil 52 is scaled from the opening shape of the entrance pupil 50 .
- the ratio of the size of the entrance pupil 50 to the size of the exit pupil 52 is defined as the opening ratio P.
- the length of the light pipe 40 is 25 mm (0.98425 inch)
- the ratio of length to width for both the entrance pupil 50 and the exit pupil 52 is 4/3 or 16/9
- the opening ratio P of the light pipe 40 is about 1.25 to 1.35.
- FIG. 7 is the position distribution of the light incident upon the entrance pupil 50 in FIG. 5.
- FIG. 7 is plotted with the transverse axis being a distance on a plane 51 A from the center of the entrance pupil 50 , and the longitudinal axis being the light intensity.
- the light pipe 40 of the present invention gathers more light 66 and leaks less light 67 in spite of the smoother light position distribution of the arc lamp 54 in comparison with FIG. 2. Because the entrance pupil 50 of the light pipe 40 of the present invention is larger than the exit pupil 52 , and the shape of the entrance pupil 52 is scaled from that of the exit pupil 50 , the light gathering efficiency of the present invention is increased.
- FIG. 8 is an incident angle distribution of the light incident upon the entrance pupil 50 in FIG. 5. As in FIG. 3, FIG. 8 is plotted with the transverse axis being the incident angle of light on the plane 51 A, and the longitudinal axis being the light intensity. As shown in FIG. 8, the incident angle of the light concentrates in the 10-14 degree range because the hyper pressure mercury light with a long arc length (Ushio, 150W, NSH150) is used in the preferred embodiment.
- FIG. 9 is the angular distribution of the light leaving the light pipe 40 in FIG. 5.
- the transverse axis is the angle of the light on a plane 51 B
- the longitudinal axis is the light intensity.
- the angular distribution is concentrated at ⁇ . Though ⁇ is larger than 14 degrees, it is far less than 30 degrees. Thus, the limitation of the incident angle for the display panel 58 is satisfied.
- FIG. 10 is the relation between the intensity of the light leaving the light pipe 40 in FIG. 5 and the opening ratio P.
- FIG. 10 shows the simulated result of the light pipe 40 of the present invention using optic simulation software.
- the transverse axis of FIG. 10 is the opening ratio P, which is the ratio of the size of the entrance pupil 50 to the size of the exit pupil 52
- the longitudinal axis is the intensity of the effective light leaving the light pipe 40 .
- the opening ratio P increases, the light pipe 40 gathers more light and the light leaving the light pipe 40 is more intense.
- the opening ratio P cannot be increased without limitation, or the angle of the light leaving the light pipe 40 becomes too large to be modulated by the display panel 58 .
- the effective light leaving the light pipe 40 becomes most intense when the opening ratio P is about 1.25 ⁇ 1.35, and therefore the light pipe 40 has the highest light gathering efficiency.
- FIG. 11 is a graph of the improvement in the light gathering efficiency of the light pipe 40 in FIG. 5 in comparison with the light pipe 10 in FIG. 1.
- the transverse axis of FIG. 11 is the opening ratio P
- the longitudinal axis is the percentage improvement of the intensity of the light leaving the light pipe 40 in comparison with that leaving the light pipe 10 , that is, the percentage improvement of the light gathering efficiency.
- the opening ratio P becomes 1.25 ⁇ 1.35
- the light intensity of the light pipe 40 of the present invention increases 6-7% in comparison with that of the prior art light pipe 10 . It is obvious, then, that the light pipe 40 of the present invention has a higher light gathering efficiency than the prior art light pipe 10 .
- the length of the light pipe 40 is 25 mm (0.98425 inches) and the arc length of the arc lamp 54 is 1.8 mm (0.0709 inches).
- the structure of the present invention can be used to optimize the light gathering efficiency by calculating the optimal opening ratio P for given light source characteristics, light collector, length of the light pipe and the arc length, etc.
- the light pipe 40 of the present invention is formed from four trapezoidal flat plates 62 .
- the area of the exit pupil 52 is smaller than that of the entrance pupil 50 , and the shape of the exit pupil 52 is scaled from that of the entrance pupil 50 . Therefore, the light gathering efficiency of the light pipe 40 of the present invention is increased within a limited space.
- Optic simulation software shows that the intensity of the light leaving the light pipe 40 of the present invention is higher than that of the prior art light pipe 10 .
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Abstract
Description
- 1. Field of the Invention
- The present invention relates to a light pipe, and more particularly, to a hollow tapering light pipe.
- 2. Description of the Prior Art
- With the progress of optics, projectors have found broad use in many applications. Generally speaking, projected light intensity is usually an important factor while designing a projector, as the projection quality improves with greater intensities of the projected light.
- Please refer to FIG. 1. FIG. 1 is a schematic diagram of a prior
art light pipe 10 for aprojector system 12. Theprojector system 12 comprises alight source 14 to generatelight 11 and to guide thelight 11 to thelight pipe 10, and animage device 16 to project the light gathered by thelight pipe 10 to ascreen 13 so as to form an image. Thelight pipe 10 is a hollow rectangular pipe set between thelight source 14 and theimage device 16 to gather and guide thelight 11. Thelight pipe 10 comprises anentrance pupil 18 and anexit pupil 19. Theentrance pupil 18 is used to gather thelight 11 generated by thelight source 14. Then thelight 11 is guided to theimage device 16 through theexit pupil 19. - Please refer to FIG. 2. FIG. 2 is a position distribution of the light incident upon the
entrance pupil 18 in FIG. 1. The transverse axis is a distance in theplane 15 in FIG. 1 from the center of theentrance pupil 18. The longitudinal axis is the light intensity. As shown in FIG. 2, the light closer to the center of theentrance pupil 18 is stronger, and the light farther from the center of theentrance pupil 18 is weaker. In addition, thelight pipe 10 does not gather all of thelight 11. Thelight 24 closer to the center of theentrance pupil 18 enters the light pipe while thelight 25 farther from the center of theentrance pupil 18 fails to be gathered by thelight pipe 10. - Please refer to FIG. 3. FIG. 3 is the incident angle distribution of the light incident upon the
entrance pupil 18. The transverse axis of FIG. 3 is the incident angle of the light on theplane 15, and the longitudinal axis is the light intensity. As shown in FIG. 3, the incident angle of a traditional light bulb is in the range of 18-20 degrees. Because thelight pipe 10 is a rectangular pipe with homogeneous cross-sections, the angle of the light leaving of theexit pupil 19 is also in the range of 18-20 degrees. Usually, the optic device for theimage device 16, such as the liquid crystal display (LCD) or the digital microscope device (DMD), has an incident angle limitation. Owing to the incident angle limitation, the angle of the light leaving theexit pupil 19 cannot be too large. Usually, light with an angle over 30 degrees cannot be modulated by the liquid crystal display. - Please refer to FIG. 4. FIG. 4 is a schematic diagram of another prior
art light pipe 20 for theprojector system 12 in FIG. 1. Thelight pipe 20, differing from thelight pipe 10, has a tapered body. Theexit pupil 23 of thelight pipe 20 is larger than theentrance pupil 22 to reduce the incident angle of the light. - Generally speaking, the
light pipes light 25 leaking from thelight pipes art light pipes entrance pupil exit pupil light 25 leaking from thelight pipe light pipes light pipe - It is therefore an object of the present invention to provide a light pipe having an exit pupil with a shape that is scaled from the shape of the entrance pupil to increase the light gathering efficiency of the light pipe, and to improve over the disadvantages of the prior art.
- The light pipe is designed for a projector system. The projector system comprises a light source to generate light and to guide the light to the light pipe, and an image device to produce an image using the light gathered by the light pipe. The light pipe is a tapered hollow tube set between the light source and the image device. The light pipe comprises an entrance pupil and an exit pupil. The entrance pupil is a square opening at one end of the light pipe. The light generated by the light source is guided to the light pipe through the entrance pupil. The exit pupil is set at another end of the light pipe, and the area of the exit pupil is smaller than the area of the entrance pupil. The light gathered by the light pipe is guided to the image device through the exit pupil. The shape of the exit pupil is scaled from the shape of the entrance pupil so as to increase the light gathering efficiency of the light pipe.
- These and other objectives of the present invention will no doubt become obvious to those of ordinary skill in the art after reading the following detailed description of the preferred embodiment, which is illustrated in the various figures and drawings.
- FIG. 1 is a schematic diagram of a prior art light pipe used in a projector system.
- FIG. 2 is the position distribution of the light incident upon the entrance pupil in FIG. 1.
- FIG. 3 is the incident angle distribution of the light incident upon the entrance pupil in FIG. 1.
- FIG. 4 is the schematic diagram of another prior art light pipe used in the projector system in FIG. 1.
- FIG. 5 is the schematic diagram of the light pipe of the present invention used in a projector system.
- FIG. 6 is a view of the light pipe in FIG. 5.
- FIG. 7 is the position distribution of the light incident upon the entrance pupil in FIG. 5.
- FIG. 8 is the incident angle distribution of the light incident upon the entrance pupil in FIG. 5.
- FIG. 9 is the angle distribution of the light leaving the light pipe in FIG. 5.
- FIG. 10 is the relation between the opening ratio and the intensity of the light leaving the light pipe in FIG. 5.
- FIG. 11 is the schematic diagram of the light gathering efficiency improvement of the light pipe in FIG. 5 in comparison with the light pipe in FIG. 1.
- Please refer to FIG. 5. FIG. 5 is the schematic diagram of a
light pipe 40 of the present invention used in aprojector system 42. Theprojector system 42 comprises alight source 44 to generate light 46 and to guide the light 46 to thelight pipe 40, and animage device 48 to produce an image by projecting the light 46 gathered by thelight pipe 40 to ascreen 64. Thelight pipe 40 is set between thelight source 44 and theimage device 48, and theprojector system 42 is a projector or a liquid crystal display (LCD). - As shown in FIG. 5, the
light source 44 comprises anarc lamp 54 to generate light 46, and alight collector 56, which is a lampshade in the shape of a half ellipsoid, to collect the light 46 generated by thearc lamp 54 and guide the light 46 to thelight pipe 40. Thearc lamp 54 is a hyper pressure mercury arc light with a long arc length 55 (Ushio, 150W, NSH150), the arc length 55 being around 1.8 mm (0.0709 inches). - The
image device 48 comprises adisplay panel 58 set on animage path 61, a plurality ofoptic lenses light pipe 40 and thedisplay panel 58, and aprojection lens 62. Thelenses light pipe 40 to thedisplay panel 58 to form the image. Theprojection lens 62 is set between thedisplay panel 58 and thescreen 64 to project the image to thescreen 64. - Please refer to FIG. 6. FIG. 6 is a perspective view of the
light pipe 40 in FIG. 5. Thelight pipe 40 is a hollow, tapering pipe constructed with four trapezoidalflat plates 62. Each of the trapezoidalflat plates 62 comprises atop end 62A, abottom end 62B, and twosides 62C. Thesides 62C of the trapezoidalflat plates 62 are joined together to from thelight pipe 40. Thelight pipe 40 further comprises four reflector walls (mirror coatings) 49 respectively set on the inner surfaces of the four trapezoidalflat plates 62 to reflect the light 46 to theimage device 48. Thereflector walls 49 absorb the infrared light in the light 46 and reflect the visible portion of the light 46. - As shown in FIG. 5, the
light pipe 40 comprises anentrance pupil 50 and anexit pupil 52. Theentrance pupil 50 at one end of thelight pipe 40 is a rectangular opening formed by the four bottom ends 62B of the four trapezoidalflat plates 62. Theexit pupil 52 at another end of thelight pipe 40 is a rectangular opening formed by the fourtop ends 62A of the four trapezoidalflat plates 62. The light 46 generated by thelight source 44 is guided to thelight pipe 40 through theentrance pupil 50, and the light 46 gathered by thelight pipe 40 is guided to theimage device 48 through theexit pupil 52. The area of theexit pupil 52 of thelight pipe 40 is smaller than the area of theentrance pupil 50, and the opening shape of theexit pupil 52 is scaled from the opening shape of theentrance pupil 50. The ratio of the size of theentrance pupil 50 to the size of theexit pupil 52 is defined as the opening ratio P. In the preferred embodiment, the length of thelight pipe 40 is 25 mm (0.98425 inch), the ratio of length to width for both theentrance pupil 50 and theexit pupil 52 is 4/3 or 16/9, and the opening ratio P of thelight pipe 40 is about 1.25 to 1.35. - Please refer to FIG. 7. FIG. 7 is the position distribution of the light incident upon the
entrance pupil 50 in FIG. 5. As in FIG. 2, FIG. 7 is plotted with the transverse axis being a distance on aplane 51A from the center of theentrance pupil 50, and the longitudinal axis being the light intensity. As shown in FIG. 7, thelight pipe 40 of the present invention gathers more light 66 and leaks less light 67 in spite of the smoother light position distribution of thearc lamp 54 in comparison with FIG. 2. Because theentrance pupil 50 of thelight pipe 40 of the present invention is larger than theexit pupil 52, and the shape of theentrance pupil 52 is scaled from that of theexit pupil 50, the light gathering efficiency of the present invention is increased. - Please refer to FIG. 8. FIG. 8 is an incident angle distribution of the light incident upon the
entrance pupil 50 in FIG. 5. As in FIG. 3, FIG. 8 is plotted with the transverse axis being the incident angle of light on theplane 51A, and the longitudinal axis being the light intensity. As shown in FIG. 8, the incident angle of the light concentrates in the 10-14 degree range because the hyper pressure mercury light with a long arc length (Ushio, 150W, NSH150) is used in the preferred embodiment. - Please refer to FIG. 9. FIG. 9 is the angular distribution of the light leaving the
light pipe 40 in FIG. 5. In FIG. 9, the transverse axis is the angle of the light on a plane 51B, and the longitudinal axis is the light intensity. As shown in FIG. 9, the angular distribution is concentrated at β. Though β is larger than 14 degrees, it is far less than 30 degrees. Thus, the limitation of the incident angle for thedisplay panel 58 is satisfied. - Please refer to FIG. 10. FIG. 10 is the relation between the intensity of the light leaving the
light pipe 40 in FIG. 5 and the opening ratio P. FIG. 10 shows the simulated result of thelight pipe 40 of the present invention using optic simulation software. The transverse axis of FIG. 10 is the opening ratio P, which is the ratio of the size of theentrance pupil 50 to the size of theexit pupil 52, and the longitudinal axis is the intensity of the effective light leaving thelight pipe 40. As the opening ratio P increases, thelight pipe 40 gathers more light and the light leaving thelight pipe 40 is more intense. However, the opening ratio P cannot be increased without limitation, or the angle of the light leaving thelight pipe 40 becomes too large to be modulated by thedisplay panel 58. As shown in FIG. 10, the effective light leaving thelight pipe 40 becomes most intense when the opening ratio P is about 1.25˜1.35, and therefore thelight pipe 40 has the highest light gathering efficiency. - Please refer to FIG. 11. FIG. 11 is a graph of the improvement in the light gathering efficiency of the
light pipe 40 in FIG. 5 in comparison with thelight pipe 10 in FIG. 1. The transverse axis of FIG. 11 is the opening ratio P, and the longitudinal axis is the percentage improvement of the intensity of the light leaving thelight pipe 40 in comparison with that leaving thelight pipe 10, that is, the percentage improvement of the light gathering efficiency. As shown in FIG. 11, when the opening ratio reaches 1.1, there is an obvious 4% improvement. When the opening ratio P becomes 1.25˜1.35, the light intensity of thelight pipe 40 of the present invention increases 6-7% in comparison with that of the priorart light pipe 10. It is obvious, then, that thelight pipe 40 of the present invention has a higher light gathering efficiency than the priorart light pipe 10. - In the above-cited embodiment, the length of the
light pipe 40 is 25 mm (0.98425 inches) and the arc length of thearc lamp 54 is 1.8 mm (0.0709 inches). In fact, the structure of the present invention can be used to optimize the light gathering efficiency by calculating the optimal opening ratio P for given light source characteristics, light collector, length of the light pipe and the arc length, etc. - In comparison with the prior
art light pipes light pipe 40 of the present invention is formed from four trapezoidalflat plates 62. The area of theexit pupil 52 is smaller than that of theentrance pupil 50, and the shape of theexit pupil 52 is scaled from that of theentrance pupil 50. Therefore, the light gathering efficiency of thelight pipe 40 of the present invention is increased within a limited space. Optic simulation software shows that the intensity of the light leaving thelight pipe 40 of the present invention is higher than that of the priorart light pipe 10. - Those skilled in the art will readily observe that numerous modifications and alterations of the device may be made while retaining the teachings of the invention. Accordingly, the above disclosure should be constructed as limited only by the metes and bounds of the appended claims.
Claims (10)
Applications Claiming Priority (3)
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TW089111241 | 2000-06-09 | ||
TW89111241 | 2000-06-09 | ||
TW89111241A | 2000-06-09 |
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US20010055098A1 true US20010055098A1 (en) | 2001-12-27 |
US6398368B2 US6398368B2 (en) | 2002-06-04 |
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US09/858,514 Expired - Lifetime US6398368B2 (en) | 2000-06-09 | 2001-05-17 | Light pipe for a projector system |
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US5884991A (en) * | 1997-02-18 | 1999-03-23 | Torch Technologies Llc | LCD projection system with polarization doubler |
JPH11142780A (en) * | 1997-11-12 | 1999-05-28 | Mitsubishi Electric Corp | Light source device and projection type display device |
CA2348386A1 (en) | 1998-10-30 | 2000-05-11 | Helen Gourley | Projector system with light pipe optics |
-
2001
- 2001-05-17 US US09/858,514 patent/US6398368B2/en not_active Expired - Lifetime
- 2001-06-07 JP JP2001172572A patent/JP2002062585A/en active Pending
Cited By (11)
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DE10242550A1 (en) * | 2002-09-13 | 2004-03-25 | Carl Zeiss Jena Gmbh | Hollow integrator for homogenizing light beams in projector comprises one-piece, hollow molding made from heavy-duty ceramic and silvered on its internal surface |
EP1577700A2 (en) * | 2004-03-19 | 2005-09-21 | LumiLeds Lighting U.S., LLC | Light emitting diode with polarised light output |
EP1577700A3 (en) * | 2004-03-19 | 2011-10-05 | Philips Lumileds Lighting Company LLC | Light emitting diode with polarised light output |
US20060126031A1 (en) * | 2004-11-20 | 2006-06-15 | Samsung Electronics Co., Ltd. | Illumination optical system of projection apparatus |
US20070165186A1 (en) * | 2006-01-13 | 2007-07-19 | Copner Nigel J | Light source system and an image projection system |
US20080019586A1 (en) * | 2006-07-20 | 2008-01-24 | Taiwan Semiconductor Manufacturing Co., Ltd. | Methods of determining quality of a light source |
US7738692B2 (en) | 2006-07-20 | 2010-06-15 | Taiwan Semiconductor Manufacturing Co., Ltd. | Methods of determining quality of a light source |
US8184896B2 (en) | 2006-07-20 | 2012-05-22 | Taiwan Semiconductor Manufacturing Co., Ltd. | Methods of determining quality of a light source |
USRE47197E1 (en) | 2006-07-20 | 2019-01-08 | Taiwan Semiconductor Manufacturing Co., Ltd. | Methods of determining quality of a light source |
USRE47272E1 (en) | 2006-07-20 | 2019-03-05 | Taiwan Semiconductor Manufacturing Co., Ltd. | Methods of determining quality of a light source |
CN102314064A (en) * | 2011-08-25 | 2012-01-11 | 北京亚视创业科技发展有限公司 | Composite light tunneling used for projector (projection apparatus) |
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