WO1995001061A1 - Moving imagery projection system - Google Patents
Moving imagery projection system Download PDFInfo
- Publication number
- WO1995001061A1 WO1995001061A1 PCT/US1994/007273 US9407273W WO9501061A1 WO 1995001061 A1 WO1995001061 A1 WO 1995001061A1 US 9407273 W US9407273 W US 9407273W WO 9501061 A1 WO9501061 A1 WO 9501061A1
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- WO
- WIPO (PCT)
- Prior art keywords
- projection system
- ught
- lens array
- viewing surface
- axis
- Prior art date
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Classifications
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N9/00—Details of colour television systems
- H04N9/12—Picture reproducers
- H04N9/31—Projection devices for colour picture display, e.g. using electronic spatial light modulators [ESLM]
- H04N9/3129—Projection devices for colour picture display, e.g. using electronic spatial light modulators [ESLM] scanning a light beam on the display screen
Definitions
- This invention relates to moving imagery projection systems and in particular to systems for projecting images and generated by computergraphic technologyformed by an intense light beam or beams on a geometric, e.g., curvilinear, domed, or spherical, viewing surface.
- the invention is particularly suitable for use in planetariums to augment existing starfields and other conventional incandescent projection devices.
- Such projection systems can not take full advantage of the seamlessness of the curvilinear viewing surface and its other inherent advantages, such as the lack of discontinuities in the image as the projection system slews the image across the viewing surface.
- Other problems with a mosaic presentation arise from imperfect seam matching, contrast or color matching, and brightness matching. Imperfections in any of these areas are readily noticed by viewers, and because even slight matching imperfections are generally noticeable on large projections, it is very difficult to eliminate these problems.
- the seamless presentation possible from a curvilinear viewing surface is easier to watch, e.g.. causes less eye strain, and creates a more realistic presentation, and continuous curvilinear viewing surfaces may also be easier to manufacture.
- a realistic ambient environmental simulation or model board image may be projected onto a viewing surface, so that a pilot or other trainee may react to it and so that the image can be altered in response to the actions and reactions of the pilot or trainee.
- CTR cathode ray tube
- CCT closed circuit television
- Such generating devices may be more suitable for mosaic presentations and suffer from the same mosaic limitations discussed above.
- the resulting image is fuzzy, blurred, or indistinct, which detracts from the training or simulation benefits of the system.
- images projected by the present invention may be similar to computergraphic images, rather than to the photo-realistic images generated by a system using CRT or CCT technology.
- a CRT system In order to avoid the resolution problems in a simulator, a CRT system must operate at a high bandwidth. The amount of bandwidth necessary increases, as the desired level of resolution increases. For example, television requires a bandwidth in the order of about 10MHz to adequately transmit the signals necessary to generate the individual points in a 625 line television picture and to repeat the picture signals twenty- five (25) times per second. In order to generate a field of view of even 175 degrees by 75 degrees, therefore, might require a bandwidth of approximately 100MHz to achieve the resolution demanded in modern flight simulation. This, however, places additional demands on the modulation of the laser beam and may make the system incompatible with digital image generating systems used in simulators.
- the present invention allows a moving image to be projected with sufficient size, intensity, and clarity to fill an entire domed or spherical viewing surface, i_e_, about 360 degrees by at least 180 degrees, and to avoid the loss of resolution and intensity experienced with other projection systems. Moreover, when the beam is static, instead of dynamic, an intense point of light is projected on the domed or spherical viewing surface.
- the computergraphic image(s) is (are) projected through a wide angle lens array.
- the wide angle lens array may comprise a single lens or a combination of lenses to achieve the wide angle projection of the images or a series of lens arrays which project the images onto a spacial image focal plane and from there through a wide angle lens or lens array onto the geometric viewing surface. It is an advantage of this feature that improved image quality can be obtained by projecting the images first onto a spacial image focal plane before projecting the image onto a domed or spherical viewing surface.
- the wide angle lens or lens array may comprise a holographic element for bending and deflecting the image forming light beams.
- the resolution and intensity of the projected image(s) is enhanced by delivering the Ught beam(s) to the wide angle lens array in an intense, coherent form.
- a source of intense, coherent light beams such as a laser, may be used and that the light beams may be provided directly to the deflector module or may be carried from the source to the deflector module by means of fiber optic cables. It is an advantage of this feature that the light source may be at a distant location from the other components of the projection system.
- the projection system of the present invention is used for projecting an image or images onto a geometric viewing surface located at a predetermined distance from and positioned at a predetermined orientation relative to the system.
- the system may further comprise a source of an intense light beam, such as a laser or an arc or a halogen lamp, e.g.. a HeNe or Argon or Krypton laser or a xenon arc lamp; a deflector module for deflecting the light beam to vector coordinates in a pair of cartesian axes; and a wide angle lens array for increasing the exit angle of deflection of the image or images from the deflector module by a predetermined factor and projecting the image or images on the viewing surface.
- the light beam may be provided directly to the deflector module or transferred to the deflector module by beam transfer means comprising a fiber optic path.
- the light beam(s) may be mono- or poly-chromatic.
- An Argon laser inherently produces two-color laser radiation. Krypton lasers, however, produce poly-chromatic radiation.
- a broadband, gas ion laser may be used to produce an intense, coherent light beam.
- a broadband laser beam includes spectrally pure, ______ discrete, and very intense frequencies.
- the broadband light beam produced by an arc or a halogen lamp includes a broad spectrum of frequencies which may be characterized by a continuous spectrum punctuated by peaks of intense frequencies. Either type of broadband light beam may be suitable for use in the invention. Further, a dye laser or other tunable laser may also be suitable for use in this invention.
- the deflector module of the projection system may comprise at least a pair of electro-mechanical deflectors which deflect the light beam to cartesian or vector coordinates in an x-axis and a y-axis. It may further comprise an x-galvanometer for deflecting the light beam in the x-axis and a y-galvanometer for deflecting the light beam in the y-axis.
- the deflector module may produce an exit angle of deflection of the deflected image in a range of about twenty (20) degrees to about eighty (80) degrees and the lens array increases the angle of deflection to a range of about 160 degrees to at least 180 degrees. At least one suitable very wide angle lens design is capable of increasing deflection up to about 210 degrees.
- the deflector module may comprise an acousto-optic or an electro-optic deflector or deflectors, which also deflect(s) the light beam to cartesian or vector coordinates in an x-axis and a y-axis.
- the wide angle lens array of the projection system may comprise a first and a second lens array, such that the first lens array projects the image or images spatially on a focal plane, and the second lens array comprises a wide angle lens and projects the spatial image or images on the viewing surface.
- the viewing surface may surround and be about equidistant from the second lens array. Further, the geometric viewing surface may be domed or spherical.
- the image or images projected by the system may be a computergraphic display defined in digital cartesian or vector coordinates which determine a trajectory for the display.
- the system may further comprise an image generating device for manipulating the display and a processor, such as an assembler, a compiler, a linkage editor, or a microprocessor, and/or a memory or data storage device for translating the digital cartesian or vector coordinates into analog signals and repetitively transmitting the display at a rate above the flicker rate.
- Flicker is a visual sensation produced by periodic fluctuations in Ught at rates ranging from about a few cycles per second to about a few tens of cycles per second i____, the flicker rate.
- the beam transfer means may also comprise a fiber optic path with an input and an output coupling for transferring the Ught beam from the source to the deflector module via a focusing and collimating lens array.
- the fiber optic path may further comprise a graded or a stepped index fiber optic cable.
- the image or images may be a computergraphic display defined in analog vector coordinates which determine a trajectory for the display. It may further comprise an image generating device for manipulating the display; a processor for repetitively transmitting the display at a rate above the flicker rate; a geometric correction device for correcting the analog coordinates, thereby compensating for the viewing surface's geometry and the distance and the orientation of the viewing surface relative to the system; amplification circuitry for controlling the deflection of the Ught beam; and beam transfer means for providing the Ught beam to the deflector module.
- the geometric viewing surface may be domed or spherical, and the second lens array may be positioned at a location about equidistant from the viewing surface.
- the image or images projected by the projection system may be a computergraphic display defined in digital vector coordinates which determine a trajectory for the display onto a curvilinear viewing surface.
- the system may comprise an image generating device for manipulating the display and a processor for translating the digital vector coordinates into analog signals and repetitively transmitting the display at a rate above the flicker rate. It also may include a geometric correction device for correcting the analog signals, thereby compensating for the curvilinear geometry of the viewing surface and amplification circuitry for controlling the deflection of the Ught beam.
- the beam transfer means may comprise a fiber optic path with an input coupling for accepting the Ught beam and an output coupling for deUvering the Ught beam to a focusing and colUmating lens array. It may further comprise a color modulator for separating the Ught beam into primary colors, modulating each of the primary colors independently, and recombining the primary colors into a single beam, whereby the amplification circuitry can synchronize the colors with the trajectory of the display.
- a poly-chromatic acousto-optic modulator PCAOM
- PCAOM poly-chromatic acousto-optic modulator
- a PCAOM employs a single acousto-optic medium, such as an acousto-optic crystal, in which each color can be manipulated separately.
- the beam may also be coupled directly to the deflector module or to the color modulator.
- FIGS. 1A and IB are block diagrams of preferred embodiments of the projection system.
- Fig. 2 is a block diagram of a preferred embodiment of the projection system depicting the projection of an image or images onto a spatial image focal plane.
- Fig. 3 is a block diagram of the x-y color modulation and deflector assembly with a optical sensor or feedback system.
- Fig. 4 is a block diagram of an electro-mechanical deflector module depicting an x-galvanometer and a y-galvanometer.
- a computer system 20 is used to generate, store, retrieve, manipulate, and display computergraphic images. These images may be generated in cartesian or vector coordinates, e.g.. along orthogonal x, y, and z axes, and may be mono- or poly-chromatic, e.g.. single color or beams of red, green, and blue (R-G-B) Ught. The images may also be manipulated to vary their intensity and orientation. In order to accomplish these purposes, computer system 20 may also comprise a keyboard, a monitor, a preview screen, a bit-pad, and a control console.
- R-G-B red, green, and blue
- suitable software should generate a time code, e.g.. simple or complex, and preferably should be suitable for use on an IBM compatible computer equipped with at least a 486 processor and operating at least 33MHz.
- image complexity is only limited by the speed of deflection, unless the speed of deflection exceeds the computer system's abiUty to generate images. For this reason, as attainable speeds of deflection increase, more powerful image generating computers may be desirable.
- Images generated by computer system 20 are transferred to a vector frame buffer processor 22 which permits the images to be repetitively displayed at a threshold rate above the flicker rate, as perceived by the human eye.
- frame buffer processor 22 translates the digital vector coordinates produced by computer system 20 into analog voltages, e.g.. voltages representing frequency, ampUtude, and geometric offset.
- the analog signals translated by frame buffer processor 22 are geometrically corrected by a geometric correction processor 24 to compensate for the extreme angles and distances between a second or spatial projecting lens array 40 having a wide angle lens and domed or spherical viewing surface 42. Without such geometric corrections, projected images might exhibit pin cushion, barrel, spherical, or other types of distortion.
- the specific geometric corrections implemented by geometric correction processor 24 are dependent upon the shape of viewing surface 42.
- a Ught source 10 for providing a beam or beams of very intense Ught may be used to produce a very smaU spot or point of Ught on viewing surface 42.
- Ught sources While a variety of Ught sources could be suitable, a broadband, gas ion laser and in particular, a broadband, KrAr laser, is preferred. This Ught source is preferred because of the coherence of the Ught beam(s) produced. It also produces a poly-chromatic Ught beam having a narrow beam diameter with extremely low divergence.
- Light source 10 is focused by means of a fiber optic input coupler 12 onto the poUshed end of a single 50/125 micron, graded index, fiber optic cable 14.
- Transmitting the Ught beam through fiber optic cable 14 achieves two purposes: (1) second lens array 40 can be positioned equidistant from domed or spherical -viewing surface 42 because Ught source 10 need not be located near lens array 40 and (2) Ught source 10 can transfer a very smaU and intense spot of Ught for projection onto viewing surface 42 with Uttle divergence or loss of coherence.
- the smaU size and focusabiUty of the Ught beam produced by Ught source 10 and transferred via fiber optic cable 14 aid in the projection of a small spot on viewing surface 42 and the rapid deflection of that Ught beam necessary to project clear images.
- the Ught beam emerges from a fiber optic output coupler 16 and enters a fiber optic collimation and focusing lens array 18.
- Lens array 18 re- collimates, e ⁇ produces a plane of paraUel Ught beams from a point Ught source, and focuses the beams.
- the beams are then directed to a modulator device (not shown), such as an acousto-optic or electro-optic modulator, which may be a component of a color modulation/intensity modulation assembly 28.
- assembly 28 may be located immediately after source 10, and the beams may be provided to assembly 28 directly from source 10 or via a fiber optic cable (not shown) while a preferred embodiment of the invention is depicted in Fig.
- space limitations in the vicinity of viewing surface 42 may dictate variations in the configuration of the system such as the relocation of components to positions distant from the viewing surface 42 by the use of optic fiber cables or other Ught transfer means or, when possible, reordering the components. See Fig. IB.
- an acousto-optic modulator is used, the ampUtude (intensity) and frequency (color) of the Ught beams entering the crystal device are modulated by the effects of acoustic waves on the crystal.
- Acousto-optic modulation is generaUy achieved by Bragg detraction, e.g.. only one usable detracted beam is produced, although other methods may be used.
- the ampUtude (intensity) and frequency (color) of the Ught beam(s) entering the electro-optic medium are modulated by the effects of electric fields on the med um.
- Electro-optic modulation may be achieved by changing the refractive index or the polarization properties of the medium by varying the appUed voltage of the electric fields. Other methods may be used to modulate the beam(s), but changing the polarization properties is preferred when an electro-optic modulator is used.
- assembly 28 After each of the primary color beams has been modulated independently, assembly 28 re-combines the beams into a single modulated beam. Signals from frame buffer 22 to assembly 28 control color selection and the intensity of the images. Moreover, frame buffer 22 helps ensure that when the beams are re-combined in assembly 28, assignment of full-color coordinates synchronized with the image's x-y axes trajectory is achieved.
- the Ught beam is then sent from assembly 28 to an x-y deflector module 30, which comprises at least two electro-mechanical, acousto-optic, or electro-optic deflectors - one for each of the x and y axes. As noted above, however, assembly 28 may be located at other positions in the system, such as immediately after Ught source /01061
- Analog signals which have been geometricaUy corrected in geometric correction processor 24, are transmitted to amplification circuitry, including a preamplifier 26 and x-power amplifier 32 and y-power amplifier 34.
- the amplification circuitry By means of signals sent from preamplifier 26 via x-power amplifier 32 and y- power amplifier 34, the amplification circuitry also controls the deflection trajectory of the images to be projected. Further, the amplification circuitry can use feedback from an optical sensing system 36 to provide accurate beam position sensing in order to correct for non-Unearities in the deflection of the beams by deflector module 30.
- sensing system 36 may operate as part of a feedback loop within the amplification circuitry.
- the exit angle of deflection of the images, after they leave deflector module 30, is in a range of about twenty (20) degrees to about eighty (80) degrees. This angle can be increased to a range of about 160 degrees to at least 180 degrees by translation of the deflected images through a wide angle conversion lens (not shown) or a short focal length lens array (not shown), such as a "fish-eye" photographic lens.
- lens array 40 should be capable of increasing the deflection of the Ught beam leaving the deflector module by a factor of about nine (9).
- a first or scan field flattening lens array 38 may be placed between deflector module 30 and lens array 40.
- Lens array 38 improves the quaUty, i_e_, decreases the size and increases the intensity, of the spot or point of Ught used to form the images on viewing surface 42.
- a beam or beams of Ught may be suppUed by Ught source 10 to a fiber positioner x-y-z adjuster 17.
- Ught source 10 is similar to that described with respect to Fig. 1A.
- Adjuster 17 aUgns the fiber optic path precisely with re-collimator 18, performing a function similar to that of fiber optic output coupler 16, as disclosed in Fig.
- Light source 10 provides a poly-chromatic Ught beam comprising the three primary colors to color modulation/intensity modulation assembly 28 to produce a full-color modulated beam of Ught.
- the Ught beam leaving assembly 28 is reflected by a beam combining dichroic filter 62 into deflector module 30.
- the Ught beam could be reflected by filter 62 into deflector module 30 after leaving lens array 18.
- a non-visible Ught beam such as a laser diode or HeNe infrared beam or a non-laser infrared beam, is generated by a non-visible Ught beam generator 60.
- the non-visible beam passes through filter 62 and is mixed and collinear with the Ught beam as it enters deflector module 30.
- dichoic filter 62 can be oriented, such that the Ught beam leaving assembly 28 passes through filter 62, and the non-visible Ught beam is mixed and becomes collinear with the visible Ught beam when it is reflected by filter 62.
- the other components of sensor system 36 would have to be re-oriented accordingly.
- x and y deflectors are driven by an analog signal processor 50 which receives x-command input 52 and y-command input 54 and suppUes command signals to x-power amplifier 32 and y-power amplifier 34.
- the beam contacts a beam separation dichroic filter 64 which allows the visible portion of the mixed beam to pass while reflecting the non-visible portion.
- the components of sensor system 36 could be re-oriented, such that the visible Ught beam is reflected, by dichroic filter 64 and the non-visible Ught beam is aUowed to pass through filter 64. As depicted in Fig.
- the fuU-color modulated, x-y deflected beam enters scan field flattening lens array 38 while the non-visible beam is reflected against an x-y position sensor 68.
- the non-visible beam passes through a position sensor enhancing lens 66 before contacting position sensor 68.
- an electrical signal is produced which is equal to the position of the non-visible beam on position sensor surface 68A. This electrical signal is summed into x-command input 52 and y-command input 54 by a four (4) quad amplifier 70 and analog signal processor 50.
- This summing detects any misaUgmnent, degradation, or distortion of the images and completes a feedback loop by which the performance of deflector module 30 can be adjusted and improved, and the deflection speed of module 30 can consequently be increased.
- FinaUy referring to Fig. 4, a preferred embodiment of x-y deflector module 30 is depicted in which electro-mechanical deflectors are employed to deflect the Ught beam in the x and y axes.
- electro-mechanical deflectors are employed to deflect the Ught beam in the x and y axes.
- an acousto-optic or an electro-optic deflector or deflectors, as weU as electro ⁇ mechanical deflectors are suitable for use with this system.
- the frequency of acoustic waves appUed to the optical medium determines the degree of deflection, usually about plus or minus three ( ⁇ 3) degrees optical.
- the method of deflection is also usuaUy Bragg diffraction, i.e.. only one diffracted beam is produced, although other methods may be used.
- electro-optic deflectors deflect Ught beams by changing the optical medium's index of refraction. By changing the index of refraction, the beams are bent in unison and are deflected, i_e_, their scan angle is changed.
- electro-optic deflectors may deflect Ught beams by changing the optical medium's polarization properties.
- a birefringent prism which spUts a Ught beam into components which travel at different velocities, may be used.
- the amount of deflection is usuaUy about plus or minus six-tenths ( ⁇ 0.6) of a degree optical, e.g.. about three (3) micro-radians per volt optical deflection. Because a preferred embodiment of the system operates at plus or minus about three thousand (3K) volts the electro-optic deflector can achieve about plus or minus about nine thousand (9K) micro-radians deflection or plus or minus about 0.516 degrees optical.
- the efficiency of acousto-optic deflectors maybe as high as about 85%. Nevertheless, when used in x-y deflector module 30, the total efficiency of deflector module 30 may only be about 30% of total Ught beam transmission.
- the efficiency of electro-optic deflectors may be as high as about 90%, and when use in x-y deflector module 30, the total efficiency may stiU be as high as about 80%, depending on the type of electro-optic interaction employed. Regardless, however, whether an acousto-optic or an electro-optic deflector or deflectors is (are) used, additional optics (hereinafter "relay optics”) may be required to obtain satisfactory results when using these deflectors in a wide angle projection system.
- relay optics are comprised of expansion and reduction optics and serve to increase system efficiency and to multiply the Ught beam deflection angles regardless of the beam's end use. As the deflection angles obtainable with acousto-optic and electro-optic deflectors continue to increase with improvements in technology, the need for relay optics is expected to diminish and possibly disappear.
- x-y deflector module 30 employs an x- galvanometer 33 equipped with an x-osciUating mirror 33A and a y- galvanometer 35 equipped with a y-osciUating mirror 35A. Electro-mechanical deflectors must be driven at relatively high speeds in order to obtain high resolution and intensity and clarity of images.
- Suitable galvanometers should have the abiUty to overcome these heat and dampening problems.
- Using a magnetic, heat transfer fluid in the galvanometers may reduce or eliminate the heat transfer and dampening problems, and improved deflector performance and greater image resolution may thereby be achieved.
Abstract
Description
Claims
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA002164443A CA2164443C (en) | 1993-06-28 | 1994-06-28 | Moving imagery projection system |
EP94920824A EP0746947B1 (en) | 1993-06-28 | 1994-06-28 | Moving imagery projection system |
DE69428716T DE69428716T2 (en) | 1993-06-28 | 1994-06-28 | PROJECTION SYSTEM FOR MOVING IMAGES |
JP50313695A JP3344587B2 (en) | 1993-06-28 | 1994-06-28 | Moving image projection system |
AT94920824T ATE207280T1 (en) | 1993-06-28 | 1994-06-28 | PROJECTION SYSTEM FOR MOVING IMAGES |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US08/082,415 US5546139A (en) | 1993-06-28 | 1993-06-28 | Moving imagery projection system |
US08/082,415 | 1993-06-28 |
Publications (1)
Publication Number | Publication Date |
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WO1995001061A1 true WO1995001061A1 (en) | 1995-01-05 |
Family
ID=22171072
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/US1994/007273 WO1995001061A1 (en) | 1993-06-28 | 1994-06-28 | Moving imagery projection system |
Country Status (7)
Country | Link |
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US (1) | US5546139A (en) |
EP (1) | EP0746947B1 (en) |
JP (1) | JP3344587B2 (en) |
AT (1) | ATE207280T1 (en) |
CA (1) | CA2164443C (en) |
DE (1) | DE69428716T2 (en) |
WO (1) | WO1995001061A1 (en) |
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- 1994-06-28 CA CA002164443A patent/CA2164443C/en not_active Expired - Fee Related
- 1994-06-28 JP JP50313695A patent/JP3344587B2/en not_active Expired - Fee Related
- 1994-06-28 DE DE69428716T patent/DE69428716T2/en not_active Expired - Fee Related
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Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO1998002863A1 (en) * | 1996-07-15 | 1998-01-22 | Carl Zeiss Jena Gmbh | Device for projection onto a dome |
WO1998015938A1 (en) * | 1996-10-09 | 1998-04-16 | Carl Zeiss Jena Gmbh | Device for the production of an image on a screen by illuminating picture elements in a plurality of partial images |
FR2754912A1 (en) * | 1996-10-09 | 1998-04-24 | Zeiss Carl Jena Gmbh | DEVICE FOR GENERATING ANNULAR SHAPE IMAGES |
DE19641657C1 (en) * | 1996-10-09 | 1998-05-14 | Ldt Gmbh & Co | Device for generating an image on a screen by illuminating pixels in a plurality of partial images |
US6169621B1 (en) | 1996-10-09 | 2001-01-02 | Carl Zeiss Jena Gmbh | Device for the production of an image on a screen by illuminating picture elements in a plurality of partial images |
Also Published As
Publication number | Publication date |
---|---|
EP0746947B1 (en) | 2001-10-17 |
CA2164443A1 (en) | 1995-01-05 |
CA2164443C (en) | 2002-04-16 |
DE69428716D1 (en) | 2001-11-22 |
EP0746947A1 (en) | 1996-12-11 |
ATE207280T1 (en) | 2001-11-15 |
DE69428716T2 (en) | 2002-07-11 |
JPH09502535A (en) | 1997-03-11 |
US5546139A (en) | 1996-08-13 |
EP0746947A4 (en) | 1997-03-05 |
JP3344587B2 (en) | 2002-11-11 |
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