EP0478568A1 - Dispositif de reproduction par projection d'images tridimensionnelles statiques ou en mouvement - Google Patents

Dispositif de reproduction par projection d'images tridimensionnelles statiques ou en mouvement

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Publication number
EP0478568A1
EP0478568A1 EP90907063A EP90907063A EP0478568A1 EP 0478568 A1 EP0478568 A1 EP 0478568A1 EP 90907063 A EP90907063 A EP 90907063A EP 90907063 A EP90907063 A EP 90907063A EP 0478568 A1 EP0478568 A1 EP 0478568A1
Authority
EP
European Patent Office
Prior art keywords
projection
images
distance
image
optical system
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.)
Withdrawn
Application number
EP90907063A
Other languages
German (de)
English (en)
Spanish (es)
Inventor
Juan Dominguez Montes
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Publication of EP0478568A1 publication Critical patent/EP0478568A1/fr
Withdrawn legal-status Critical Current

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Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS 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
    • G03B35/00Stereoscopic photography
    • G03B35/18Stereoscopic photography by simultaneous viewing
    • G03B35/24Stereoscopic photography by simultaneous viewing using apertured or refractive resolving means on screens or between screen and eye
    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03BAPPARATUS 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
    • G03B35/00Stereoscopic photography
    • G03B35/18Stereoscopic photography by simultaneous viewing
    • G03B35/20Stereoscopic photography by simultaneous viewing using two or more projectors
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N13/00Stereoscopic video systems; Multi-view video systems; Details thereof
    • H04N13/30Image reproducers
    • H04N13/302Image reproducers for viewing without the aid of special glasses, i.e. using autostereoscopic displays
    • H04N13/305Image reproducers for viewing without the aid of special glasses, i.e. using autostereoscopic displays using lenticular lenses, e.g. arrangements of cylindrical lenses
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N13/00Stereoscopic video systems; Multi-view video systems; Details thereof
    • H04N13/20Image signal generators
    • H04N13/204Image signal generators using stereoscopic image cameras
    • H04N13/207Image signal generators using stereoscopic image cameras using a single 2D image sensor
    • H04N13/229Image signal generators using stereoscopic image cameras using a single 2D image sensor using lenticular lenses, e.g. arrangements of cylindrical lenses

Definitions

  • This invention describes a device capable of reproducing static or moving three-dimensional images by projection using ordinary light.
  • stereoscopic is used for systems in which
  • the term three-dimensional is used to distinguish the systems that use a greater number of captured and reproduced images, allowing observation within a wide viewing angle, without disturbing
  • the holographic technique is based on wavefront reconstruction photography. These systems require the coherence of the light sources of
  • the acquisition is made through two objectives separated from each other by a distance, approximately equal to the average value of the distance between the eyes of human beings.
  • stereoscopic systems in which the arrival of a different image to each eye is achieved through procedures not suitable for projection.
  • these are those who interpose, between the observers and the reproduced image, an optical system, such as that of Breter's prisms and that of Wheatstone's flat mirrors, ⁇ orling, JA, The Stereoscopic Art. ... A. Reprint. J. Smpt 60, u '3, 286-308 (March 1953) 7, or Kempf's concave mirror, US Pat.
  • the stereoscopic systems suitable for projection are very varied depending on the procedure used to convey the image captured by the left lens to the left eye and the image captured by the right to the right.
  • the best known and most used in stereoscopic projections with movement are those that use colored, polarized or shutter filters.
  • stereoscopic systems used in projection, is that they need to disturb the observer by placing optical filters or a shutter mechanism in front of them.
  • US Patent 4,086,585 to Wah-Lo describes a system and camera for controlling depth of field in three-dimensional photography.
  • the diffusing surface is made of an opaque material if the projection is front or a translucent material if the projection is rear. In all cases the images appear on this surface divided into thin vertical strips.
  • Patent 1,883,290 by Ivés which describes a frontal projection procedure on an opaque screen in which the element that divides the image into fine vertical strips is the same sheet of vertical cylindrical lenses through which it is carried out. the observation, and another of rear projection on a translucent surface in which the element that divides the images into thin vertical strips is also a sheet of vertical cylinders used in the process of copying the different films into one.
  • a high precision adjustment is required to position the image strips on each cylinder.
  • the maximum angle of view is limited by the opening of the vertical cylinder, the relation between its width and its focal length; If this angle is exceeded, the observation is made on a strip of image corresponding to the attached cylinder, producing the undesirable pseudoscopic effect, that is, the inverted depth.
  • Haisma in his aforementioned patent, (see 10 pp. 1-65) highlights the importance of this problem.
  • the first increasing the size of the reproduced image, can be seen on p. 3, 58-65.
  • This procedure there is a loss of quality in the reproduction, derived from the fact that the distance between the axes of the cylinders is greater than the diameter of the cylinders, consequently, dark vertical strips appear between cylinders, see Ivés'290 p. 3, 65-75.
  • the enormous manufacturing complexity of this lenticular sheet is obvious.
  • the second based on the relative decrease in the focal length due to an increase in the refractive index, leads to the need to place opaque sheets between cylinders, making their manufacture notably complicated (see Ives'290 p. 4, 45-50). .
  • Image quality is limited by the transverse dimension of the cylindrical lens, which in turn is limited by that of the vertical fringe of the image.
  • each vertical image strip must be as many times less than the size of the cylinder as the number of images reproduced. For this reason, the size of the cylinder is limited by that of the image, which, in turn, is smaller than that of said cylinder.
  • the non-observance condition of a strip of width "d" for a healthy eye is that
  • each image strip must be 0.03 and 0.008 mm. , respectively. These values are of the order of only 15 times greater than the wavelength of visible light. If a number of images greater than 10 were used, the situation would logically be aggravated. Manufacturing difficulties are obvious and, therefore, the price of the marketed product is high. In systems like Haisma, the image is positioned through optical conductors, this difficulty can be insurmountable.
  • the invention is due to Lippmann, a famous French optician in 1908 (Lippmann, M.g., Epreuves Repreuves Rversibles Donnant la Sensation du Relief. J. Phys. 7, 4th series, 821-825 (Nov-1908)).
  • the basis of integral photography is to prepare a sheet of fly-eye lenses, made of glass or plastic, with a tremendous number of spherical plano-convex lenses (for example 10,000).
  • Haisma in its patent n ⁇ 4,571,616, already mentioned, describes an integral relief system based on the capture of the image by conventional cameras that form a square mosaic. He gives as an example a number of 9 cameras arranged in 3 columns of 3 cameras each.
  • Reproduction is carried out by positioning, behind each spherical lens, nine different pieces of images, at the rate of one piece for each image captured. Adjustment is achieved by properly positioning the optical conductors by mechanical means. If the manufacturing complexity involved in placing n image strips behind each cylinder has been seen before, the problem here is much more serious, then,
  • Yano in the second part of his patent for USA 4,078,854, replaces the diffuser surface with a sheet of horizontal cylindrical lenses, but does not do so to design a new system based on the angular differentiation of images, but rather as a mere variant of the one described in the first part and based on in scalar differentiation on a diffusing surface in translucent material.
  • the system is called stereoscopic reproduction in that patent, having a very small number of reproduced images (see pages 1, 10-13) that can be a maximum of five (see pages 5, 30- 32) with a wide margin of vision, but, as is recognized in that patent (see pages 3, 32-36), there are observers who will see the same image with both eyes and for which it is needed give a sense of depth by other means.
  • this last device described has two elements, a convergent optical system that conditions and hinders the projection of large images and a screen composed of two cylindrical lens sheets; the opening of the cylinders has a concrete and fixed value independent of the distance between objectives-projectors and the projection distance; which shows that its design is not based on the angular differentiation of images.
  • the system object of this invention is based on the angular differentiation of images, for which, in addition to suppressing the diffusing surface, it is necessary to conceive the reproduction of images in a different way from that carried out in previous systems.
  • each observation point In a system based on the angular differentiation of images, from each observation point only one rectangle is seen of each image, which will be -distinct for each observation point.
  • the set of rectangles corresponding to an observation point will form a unique and different image from the one corresponding to any other point.
  • the photons from the different projections retain their direction after passing through it.
  • the different images can be distinguished because the photons of each emerge at a different angle from this transparent surface: that is, "Angular image differentiation" can be used.
  • an optical frame of vertical cylinders will first be placed in front of this transparent surface and at a distance equal to the focal length of these cylindrical lenses.
  • the choice of the focal length of these cylindrical lenses is made in such a way that the ratio of the cylinder's transverse size to its focal length is at least equal to the ratio of the distance between two projection lenses adjacent to the projection distance, and never more than double that value.
  • any observer whatever their position, will see as many image segments as there are projection targets. These will be aligned in a single rectilinear segment. This rectilinear image segment will be different for each observation point and will be contained in the line resulting from the intersection of the plane, which contains the projection objectives and the observer, with the transparent projection surface.
  • the projection objectives will be located in a horizontal line and a second optical frame of horizontal cylinders, whose focal lines are in the same focal plane of the vertical cylinders. and, therefore, coinciding with the transparent screen devised with pedagogical units, it will be in charge of converting the previous segment into a rectangle, whose base will be the size of this same segment and whose height will be that of the transparent surface.
  • a different image rectangle will correspond to each observation position and the set of these rectangles will form a unique and different image for each observation point.
  • the focal length of these horizontal cylinders must be as small as possible compared to their width (semicircular cylinders), in order to ensure that their opening allows the vision, from any point, of a rectangle as high as the optical system itself. .
  • the optical system object of this invention consists of two sheets of cylindrical lenses per pendicular to each other and such that the resulting vertical optical aperture encompasses at least two vertical projection objectives and at most three and the optical aperture.
  • the resulting horizontal ca encompasses at least two horizontal projection targets and a maximum of three.
  • the system thus designed is made up of cylinders with a very small opening, that is to say, with a very large radius relative to their transverse size.
  • This small aperture value is also independent of the orthoscopic viewing angle.
  • the size of the cylinders as it is a system based on the angular differentiation of images, is independent of the number of images reproduced and by both the quality of the reproduction can be very high. By not using an additional convergent optical system, large images can be reproduced without difficulty.
  • Frontal projection is achieved by simply replacing one of the lens sheets with mirrors, without the mirror image of the projectors appearing at any time. Rear projection does not require special precision adjustments and each observer sees a different image with each eye. In short, the advantages of this system over all other systems are:
  • the orthoscopic viewing angle can be made as large as desired, it only depends on the number of projectors, the distance between them and the projection distance.
  • the size or width of the cylinders is not limited by the number of images and can be designed as small as desired, so the image quality is only limited by the manufacturing conditions of these cylinders.
  • Figures 1, 2 and 3 explain the ideas on which the new system is based, while Figures 4, 5 and 6 describe the system that is the object of this invention.
  • - Figure 1 shows the horizontal parallax angle E with which an object P is seen at distance 1 from an observer with a distance b between his eyes.
  • FIG. 2 schematically shows an observer 0-, looking at an object P through the window AB.
  • FIG. 3 schematically shows m observers 01, '02 ... 0 m m looking at an object P through the window " AB.
  • FIG. 4 shows n cameras CC- ,, ⁇ C 2 ... CC separated from each other by a distance K and with their optical axes parallel.
  • FIG. 5 shows the arrangement of the projection objectives PR- ,, PR ... PR and of the optical frame of vertical cylinders (1) of focal length f and transversal size d. '
  • the distance between two adjacent projection lenses is K R and the projection distance B.
  • FIG. 6 shows the optical system object of this invention from which the optical frame of vertical cylinders (1) can be seen, in its front part, in its rear part the optical frame of horizontal cylinders (2); where "e” is the thickness of the system V the angle of view, S the horizontal angle under which two projection lenses are seen, f the focal length of the vertical cylinders, B the projection distance, K R the distance between two projectors contiguous and ER ] _, Hi2 ... the situation of the optical centers of the you of projection.
  • Binocular vision is what allows us to appreciate the distance at which objects are. This operation is carried out by means of the angle that the eyes rotate. Let the lines I1A1 and D1A2 be the infinity vision lines of the left eye II and the right eye DI respectively. Reference is made to Figure 1 which schematically represents the binocular observation of an object P. If the eyes rotate to observe an object P located at a distance 1 on the line I1A1, the right eye will do so. in an angular magnitude E given by the expression
  • Angle E is called the horizontal parallax angle.
  • the systems that reproduce this parallax are sufficient and satisfactory. For this reason, the capture and reproduction of horizontal parallax constitute the essential part of three-dimensional vision based on the angular differentiation of images, as explained below.
  • This figure 2 shows this 0- observer in plan, with his right eyes D-, and left eyes I-,.
  • the beam of light rays that, starting from the landscape, pass through 1 ⁇ is the one that serves to form the image of the left eye.
  • the beam of light rays, passing through D- , serves to form the image of the right eye.
  • the perception of relief is achieved when the brain synthesizes the images of the left and right eyes, formed by these two beams of light rays, ⁇ which pass through points I-, and D-, not coincident.
  • the line AB contained in the trace of the plane that contains the window, is considered decomposed into the series of infinitely close points F- ,, F ? ... F .... F ,,
  • every ray belonging to the homocentric beam I-, as well as every ray belonging to the homocentric beam D-, are contained in the set of homocentric beams F ⁇ i, F ._... Fi. ... Fn - l,, 'Fn, as long as the distance - ⁇ - ? ⁇ * ⁇ - ! _ ⁇ for any i is small enough.
  • Figure 3 represents the optical scheme of m observers looking at an object through window AB.
  • the image formed based on the homocentric beams I. or D. corresponding to the left and right eyes of observer 0., and for any observer 0., can be synthesized by selecting and conveniently composing pieces of the images formed by taking as a basis the homocentric beams F. ,, F ... F .... P - ,, F provided that the distance ⁇ A ⁇ ®- ⁇ _- ⁇ is small enough ".
  • the minimum necessary separation (or size of the reproductive elements) are very different, so as not to appreciate that the image is made up of stripes, and the necessary separation (or distance between optical centers of objectives in the capture), to be able to reproduce in an apparently continuous way the variation of parallax.
  • the method object of this invention such as shutter in cinematography, allows that, with a small number of captured images, it can be reproduced with a large number of elements.
  • the same image is repeated during several shutters.
  • three-dimensional reproduction the same image will be repeated in several reproducing elements.
  • the maximum distance between the optical centers of the camera lenses is imposed, for each depth of field, by the condition of image continuity in the reproduction. This condition is the same for all three-dimensional reproduction systems of the prior art and for that of this invention.
  • the distance between the adjacent optical centers of the projectors, when using the angular difference of images, is determined by the relationship between the projection aperture and the observation aperture.
  • the projection aperture is the quotient between the distance between the optical centers of two adjacent projection lenses and the projection distance.
  • the observation aperture is the quotient between the distance between the eyes of an observer and the observation distance.
  • Our experience has shown that three-dimensional vision with angular differentiation of images is acceptable even for projection aperture values three or four times higher than those for observation.
  • the distance between targets in the capture can be much greater than the distance F.-F ._-
  • the capture procedure will consist of a series of capture targets whose optical centers are on a horizontal line separated from each other at a distance Kc that will be a function of the depth of the capture field.
  • this procedure has been schematically represented.
  • each objective belongs to a different camera and that the optical axes of these objectives are parallel to each other.
  • the objectives can belong to a single camera and the optical axes can be tilted.
  • CC- ⁇ CC 2 , CC., ... CC n are the n cameras with the optical centers of the objectives separated by a distance Kc and located on the horizontal line ZZ '.
  • the same number of projector lenses will be used in the projection as the number of camera lenses used in the shot. Each of them will project an image on a transparent optical-cylindrical screen.
  • Figure 5 schematically represents the arrangement of the projection objectives PR- ,, PR 2 ... PR n separated from each other by the distance KR projecting onto the optical-cylindrical reproduction screen.
  • each objective has been represented as belonging to a single project and to all the parallel optical axes.
  • the optical axes may be inclined. It is important to bear in mind that the angle formed by the different image films in the projection must be the same as that formed by the images. image lines in the uptake. Otherwise, flat surfaces of equal parallax in the capture will be reproduced as curved surfaces in the reproduction, unless a compensatory inclination is introduced in the process of copying the films.
  • the distance B from the projectors to the screen is dictated by the focal length of the projectors and the size of the screen or optical-cylindrical frame.
  • the optic-cylindrical plot (1) is made up of cylinders with a width d, small enough not to be perceived, experience tells us that for a healthy eye the width d of the cylinder should be less than the viewing distance in meters divided by 3,500.
  • the opening of the cylinder can be between this value, vision covering three projection objectives, and its half, vision covering two projection objectives. This achieves an imperceptible transition of an image fringe to the following, since the image part of the projection objective PRi mixes smoothly with that projected by its neighbors FR. ⁇ and -PR i + 1 »
  • the reproduction parallax decreases although the three-dimensional and reverse angle of view increases.
  • the projection lenses are separated from each other, the reproduction parallax decreases although the three-dimensional and reverse angle of view increases.
  • the projection distance is maintained, there will correspond to of a different cylindrical screen, since it is necessary to make the relation between transversal size and focal distance of the cylinder equal to the relation between distance between projection objectives and projection distance.
  • the vision of the images would be limited to a rectilinear segment composed of as many sub-segments as images or projection objectives. This rectilinear segment is given by the intersection of the plane that passes through the projection objectives and the observation point with the plane that contains the aforementioned transparent optical frame of vertical cylinders.
  • the optical reproduction system will be as shown in Fig. 6 and its vision will be made by transparency.
  • the angle of view V can be seen, which is a function of the quotient between the separation distance from the first projection objective to the last projection objective, and the projection distance B.
  • the angle S can be considered of opening of the vertical cylinders, function of the quotient between the separation between two contiguous projection objectives K R and the projection distance B, coefficient that is the same as that obtained between the transverse size of the vertical cylinder d and its distance focal f.
  • the thickness of the optical system must be:
  • e (r 2- r l ⁇ nl where r 2 and r 1 are the radii of the vertical and horizontal cylinders respectively and n is the refractive index of the substance with which the optical system is made.
  • the same bases that have served to create a three-dimensional reproduction system with variation of the horizontal parallax are valid for the design of an "integral reproduction system", a system that reproduces horizontal and vertical parallax. simultaneously.
  • the projection objectives will be arranged in this case on a rectangle.
  • the design of the horizontal cylinders (2) is made in a similar way to the design of the vertical ones.
  • the ratio of the cylinder's transverse size to its focal length is at least equal to the ratio of the distance between three vertical projection lenses to the projection distance.
  • optical characteristics such as being lenses or mirrors, optically convergent or divergent, can be chosen arbitrarily.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Testing, Inspecting, Measuring Of Stereoscopic Televisions And Televisions (AREA)
  • Stereoscopic And Panoramic Photography (AREA)

Abstract

Dispositif pour reproduire par projection des images tridimensionnelles statiques ou en mouvement, dont la prise s'effectue au travers de plusieurs objectifs, situés chacun d'eux dans une position spatiale distincte; dans le système de reproduction, il n'est pas besoin de distinguer les différentes images par leur position étant donné qu'elles ne sont pas reproduites sur une surface de diffusion; la projection s'effectue directement sur un système optique transparent, la distinction entre les images se faisant par leur angle de projection; ce système optique se compose d'une feuille de lentilles cylindriques verticales dont la taille transversale n'est pas conditionnée par le nombre d'images et dont l'ouverture est indépendante de l'angle de vision orthoscopique et d'une feuille de lentilles cylindriques horizontales de distance focale courte et de dimension arbitrairement petite et formant un système de reproduction facile à fabriquer et adaptable à n'importe quel angle de vision pour donner une image distincte en chaque point d'observation.
EP90907063A 1990-04-23 1990-04-23 Dispositif de reproduction par projection d'images tridimensionnelles statiques ou en mouvement Withdrawn EP0478568A1 (fr)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
PCT/ES1990/000014 WO1991016664A1 (fr) 1990-04-23 1990-04-23 Dispositif de reproduction par projection d'images tridimensionnelles statiques ou en mouvement

Publications (1)

Publication Number Publication Date
EP0478568A1 true EP0478568A1 (fr) 1992-04-08

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EP90907063A Withdrawn EP0478568A1 (fr) 1990-04-23 1990-04-23 Dispositif de reproduction par projection d'images tridimensionnelles statiques ou en mouvement

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EP (1) EP0478568A1 (fr)
JP (1) JPH04501922A (fr)
WO (1) WO1991016664A1 (fr)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2358980B (en) 2000-02-07 2004-09-01 British Broadcasting Corp Processing of images for 3D display

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR750156A (fr) * 1932-01-23 1933-08-05 Procédé de photographie et de cinématographie d'images polychromes à effet plastique
US4078854A (en) * 1971-10-05 1978-03-14 Canon Kabushiki Kaisha Stereo imaging system
ES2000293A6 (es) * 1986-12-29 1988-02-01 Dominguez Montes Juan Instalacion y procedimiento para obtener imagenes tridimensionales en movimiento esto es tetradimimensionales tanto en color como en blanco y negro

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WO1991016664A1 (fr) 1991-10-31
JPH04501922A (ja) 1992-04-02

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