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Número de publicaciónWO1987007383 A1
Tipo de publicaciónSolicitud
Número de solicitudPCT/US1987/001279
Fecha de publicación3 Dic 1987
Fecha de presentación29 May 1987
Fecha de prioridad30 May 1986
También publicado comoEP0267956A1, EP0267956A4
Número de publicaciónPCT/1987/1279, PCT/US/1987/001279, PCT/US/1987/01279, PCT/US/87/001279, PCT/US/87/01279, PCT/US1987/001279, PCT/US1987/01279, PCT/US1987001279, PCT/US198701279, PCT/US87/001279, PCT/US87/01279, PCT/US87001279, PCT/US8701279, WO 1987/007383 A1, WO 1987007383 A1, WO 1987007383A1, WO 8707383 A1, WO 8707383A1, WO-A1-1987007383, WO-A1-8707383, WO1987/007383A1, WO1987007383 A1, WO1987007383A1, WO8707383 A1, WO8707383A1
InventoresDonald A. Clarke, Roger Reynolds, Timothy R. Pryor
SolicitanteDiffracto, Ltd.
Exportar citaBiBTeX, EndNote, RefMan
Enlaces externos:  Patentscope, Espacenet
Index-sight
WO 1987007383 A1
Resumen
Method and apparatus for rendering visible changes in a refractive media such as gas and fluid flows which cause changes in the index of refraction due to pressure or thermal gradients, detection of leaks and distortion in window glass. In one embodiment the medium (15) whose deviation in index of refraction is to be determined is located between a point light source (10) and retroreflective screen (20). A camera (30) is focused to make the effect visible.
Reclamaciones  (El texto procesado por OCR puede contener errores)
WHAT IS CLAIMED IS:
1. A method for visualizing distortions in media comprising: illuminating a retroreflective material composed of a large nuπfcer of snail reflective elements with light fran a light source, said light travelling to said material via said media, and viewing said retroreflective material through said media from a position angularly proximate said light source to determine said distortions from the dark and/or bright indications produced.
2. A method according to Claim 1 wherein said media are of differing indices of refraction than the surrounding media through which said light also travels.
3. A method according to Claim 2 wherein the presence of said distortions indicates the presence of said media, as in leak testing.
SUBSTITUTE SHE TS'
4. A method according to Claim 2 wherein the indices of said refraction of said media are varied by thermal, pressure or density effects whose presence, magnitude or distribution are to be determined.
5. A method according to Claim 1 wherein .said media are of substantially constant and uniform index of refraction, but geometrically distorted locally so as to produce said distortions.
6. A method according to Claim 1 wherein said distortion is observed by a TV camera.
7. Apparatus for rendering visible distortions in a media comprising: light source means for illuminating said media; and retroreflective material means for returning light pass.
Descripción  (El texto procesado por OCR puede contener errores)

r

INDEX-SIGHT

FIEID OF THE INVENTION

This is a continuation-in-part of copending PCT applications Appln. No. US85/00125 (corresponding to U.S. Patent No. 4,629,319) and Appln. No. US86/00519, the disclosures of which are incorporated by reference herein. Those applications relate to a unique method for observing deviations in geometric forms of surfaces. This technique is hereby extended to the examination of variations in index of refraction caused by similar distortions and disturbances in fluids such as air, gases and glass. This new version is called "Index-Sight", and is a continuation-in-part of the previous efforts called "DiffractoSight".

DESCRIPTION OF THE PRIOR ART

Researchers in fluid mechanics often use flow visualization techniques to qualitatively determine how fluids mix together, flow over obstructions, or pass through orifices restricting such flow, etc. Similarly, researchers in heat transfer use flow visualization to study heat transfer through barriers and via heat sinks attempt to identify sources of heat loss and the like.

Typical systems used in the prior for the visualization of index of refraction have included shadowgraphs, Schlieren effect systems and others.

A shadowgraph such as shown in Figure 1A is a device used to generate a colli ated beam of light from a source S using a lens LI over a test section sufficiently large to accommodate a model 0 of the physical system being examined. This field of light is then collected using lens L2 so that it can be projected or imaged as an image I onto a screen. Figure 1A shows such an arrangement typical of the shadowgraph and Figure IB shows such an arrangement typical of the Schlieren device used to study shock wave phenomena.

In the Schlieren arrangement, the image I from lens L of the light source S is removed using a knife edge 8 near the focus of the field mirror M2 such that only the optical perturbations (for example, due to the pressure and temperature change in compressible fluids in object 0) can be observed. In both cases, mirrors Ml and M2 are normally used to compensate for the prohibitive cost of large

TE SHEET- lenses. These mirrors are usually c-anted, which contributes to optical parallax. Models must be used since the cost of large lenses or mirrors makes real object sized test fields expensive. Variations in fluid density due to changes in pressure, temperature or type of fluid mixing with the host, result in variations of refractive index. This in turn causes the light to image at variable locations and a visual two-dimensional record of the effects results. Typical references are included for flow visualization.

The Scientific American article referenced below (April/86) shows a means for on-axis illumination with a retroreflecting screen used for the purpose of removing noise in an optical path. This arrangement introduces a point light source with a beam splitter to achieve

_ϋ.lumination and imaging on the same axis. The object or system generating the optical disturbance(s) must be placed close to the retroreflecting screen in order that the optically encoded signal is decoded by passing back along essentially the .same light path. This filters out the offending optical noise.

The 3M Technical Service Bulletin Industrial Optics #34-7016-4250-5 describes installation instructions and on the last page shows guidelines for equipment and screen placement for photographing an object with a superimposed background. The background is projected from a large format projector onto the retroreflective screen through the beam splitter shown. The object would be located close to the retroreflecting screen so that both object -and background can be in focus and the composite scene imaged on axis by the camera looking through the be^am splitter. Because the projector is not a small light source, the effects of index changes in the light path cannot be resolved easily. As well, index effects will be further minimized having the object close to the screen.

Related art for this invention occurs in other fields. As disclosed in recent literature, atmosphere distortion of images can be corrected by placing retroreflective material such as that used herein directly and immediately behind the disturbing medium. See Walker, J. "Wonders with the retroreflector, a mirror that removes distortion from a light beam", Scientific American, Vol.254, No.4, April 1986 at 118.

SϋMMAIff OF THE INVENTION

With the present invention, startling results have been obtained. With simple equipment, it is possible to visualize effects including (but not restricted to) changes

SUBSTITUTE SHEET in refractive index surrounding one's head or arm in normal ~oo~. environments. The technique particularly utilizes a retroreflector material such as -Scotchlite 7615 manufactured by 3M making possible the application to large fields of view. Such material is typically comprised of large numbers of small retroreflective elements such as reflective glass beads.

In comparison with prior art wind tunnel shadow graph techniques, there are some similar effects produced. However, the disclosed invention is much more energy efficient and further is capable of irradiating much larger areas since there is no requirement for large lenses, mirrors or the like. In addition, it requires very little alignment and is capable of much easier set up and use.

BRIEF DESCRIPTION OF THE DRAWINGS

Figures 1A and IB illustrate the prior art in the form of shadowgraphs (Fig.1A) and Schlieren effect (Fig. IB) used for examination of fluid flow.

Figures 2A and 2B illustrate a two dimensional and three dimensional system according to the invention for rendering visible thermal waves from a human arm utilizing a substantially point source and TV camera. Such waves are also visible using the human eye directly, and can be recorded by me-ans such as photographic film, etc.

Figures 3A and 3B illustrate alternative off-axis and on-axis optical arrangements of the invention. Figure 4 illustrates an application of the invention to monitoring turbulence of airflow near airfields.

Figure 5 illustrates an application of the invention to the inspection of glass panes.

Figure 6 illustrates an application of the invention to the determination of leaks in car bodies.

Figure 7 illustrates the detection of water waves.

DESCRIPTION OF THE INVENTION

Figures 2A and 2B illustrate a substantially point light source 10 located near the eye 11 of the observer, or a camera 30, used to obtain the data.

The medium 15 in this case is air near a human arm 16 whose deviation in index of refraction is to be determined. The medium 15 is arranged to be between the camera 30 and the retroreflective screen 20, which are preferably distant from each other so that maximum optical leverage occurs. The camera system 30 (or eye 11) is focused to make the effect visible. It is generally preferable to have the image of the screen 20 substantially in focus.

SUBSTITUTE SHfiKT It is essential that the medium 15 be remote from the screen 20 so that the deviations become manifest. While effects can be noticed -as close as one (1) foot (1/3 m) , best results occur at distances over 1 meter. For example, in the experiment depicted in Figs. 2A and 2B, the distance LI from the screen 20 to the human arm 16 was 10 meters (30 ft.) , while the distance L2 from the camera 30 to the person's arm 16 was 6 meters (20 ft.) . It is also generally preferable that the light source 10 be substantially a "point" source, for best resolution of minute index change related fluctuations.

When this image is taken with the camera 30, the heat waves rising from the person's arm 16 are made visible. That is, the air medium 15 has been heated by the person's arm 16 and becomes distorted from its normal quasi-homogenous state. Ideally, a camera such as 30 can be utilized with a telephoto lens whose field of view substantially encompasses the screen 20 and/or medium 15 whose distortion is to be examined. This allows for clear discernment of index gradient effects including the heat waves which occur when a thermally variant object radiates into its surroundings.

In one embodiment of the invention, images are produced with the light source 10 directly along the axis of the

SUBSTITUTE SHEET camera 30. This can be accomplished by either a beam splitter 22 and light source 19 or by placing a small point light source, such as a fiber optic, in the middle of the lens. Alternatively, a substantially off-axis arrangement 40 can also be used as shown in Fig. 3A. Where the distance H is large, the shadow 42 of the object 44 falls on the screen 46 as shown, but the camera 48 does not see the direct image of the object 44. Interestingly, in this case if the object is, for example, a butane fuel lighter, the fuel coming out of the lighter can be seen as an index change but the flame •. can be seen only in the direct image.

Unlike the previously disclosed DiffractoSight reflective effect described in the above-identified patent where there is a definite preference in practice for off-axis illumination, the herein described effect, generally speaking, appears to work best on-.axis. The near off-axis (H small) condition is, however, easier to arrange experimentally since the light source 50 can be off to the side. Indeed one can even have an image which only results essentially from the shadow 42 of the object 44 and not the backlit object itself.

For example, in practicing the invention, it has been found that a possible alternative arrangement is to locate

SUBSTFFU the light source 50 off the axis of the camera unit 48 such that the shadow 42 (so to speak) of the object 44 falls onto the screen 46 but with the object 44 itself not being directly in the field of view of the camera 48 (Fig. 3A) . In such a case, one sees the shadowed effects caused by the variations in index which are typically light and dark zones due to the deformation of the light waves passing through the index variant medium. This arrangement includes warmer air rising from the surface of the ground. For longer wavelength variation, however, it may well be that of-axis illumination is best, as in the "example on slowly changing sheet metal surfaces discussed subsequently. An example herein is glass defects such as waves caused by the float glass process or other curvature defects due to distortion of the glass itself.

Also in this category are long wavelengths on the surface of water which can be illuminated both in reflection as to the previous disclosures or in refraction as in this disclosure creating virtually the same kind of a refractive low -spot or high spot as has been seen on sheet metal for example (see Fig. 7) .

As disclosed in the referenced copending applications, it is also possible to computer-process the image to find the changes in index, distortions in glass, or other variables. High speed photographs can also be taken using strobes, electronic images, cinema cameras, or the like. Processing can be used to compare the image of the object index patterns to master stored images as well as to determine the gradient across the image in real time or after the fact. Recording devices such as film, videotape, disc, etc., can be used to record images produced for later analysis.

There are numerous additional applications proposed for this invention. Pressure gradients accompanying wind shear is an interesting idea. For example, consider Figure 4 wherein a substantial zone area along (or near) an airport runway 301 is covered with retroreflective material 302. This retroreflective material 302 is then viewed by the pilot 304 on approach using a point light source 306 (such as a landing light) and produces information regarding the wind shear characteristics which may be present in the flight path. This can also be caused by turbulence from preceding aircraft as well. Another application is in the detection of fluid leaks, including the butane lighter example hereabove. This would be useful in transportation applications where a fluid of a different refractive index could be introduced into the body of a vehicle in order to see leaks that emanated therefrom

SUBSTI (e.g, from a bad door seal) . In this case, the leaking would be immediately apparent and this obviates using costly helium "sniffers" on robots or the like.

Another application is in determining over large expanses the presence of potential fires or overheating components in areas, electrical devices, etc. Another is studying air flow in air conditioner or heating ducts, pipes or other heat transfer situations. The sole requirement is to create a refractive index change which can be detected with the invention.

The on-axis version of the invention appears to produce light and dark shadows on the screen, such shadows corresponding to positive or negative gradients of index. When one moves the light off-axis, there is an apparent change in the type of phenomenon being examined in respect of the positive gradients, such change being different but related. As in the preceding applications, it seems likely that the positive and negative going slopes of the refraction surface are being resolved differently. Depending on the offset direction of the light source from the c-amera, the viewing angle slope is either positive or negative going.

An analogous case, for example, is depicted in Figure 5 wherein waves 60 in the surface of and within a piece of glass 61 are visualized using a light source 64, a screen 66, and a TV camera 68. Such waves 60 are typically within 2 in. (5 cm) in wavelength and are visible in reflection as well. (See window glass "ripple" in the DiffractoSight photograph in the above-mentioned patent) .

Figure 6 illustrates such an embodiment of the invention, used for leak tests on vehicles 70. A very important task in the production of vehicles 70 is to ascertain the structural integrity of numerous door, window and body seals. Le-aks occurring in transmission cases, engines, cylinder blocks/oil pans and the like are similarly important. However, the major leak tests of interest relate to the passenger area.

For this it has been known in the prior art to fill the vehicle with a gas such as Freon and "sniff" this with a gas detector carried by a robot. Other proposals such as acoustics and the like have also been investigated.

It is proposed herein to fill the vehicle 70 with gaseous helium, Freon or the like gas 74 such that a difference in refractive index between the introduced gas 74 and the ambient air is thereby created. Human vision or TV camer.as 72 can examine the vehicle 70 as it passes by or rests in a fixed position adjacent a screen 78 to check for a leak 82. Ideally, such gas 74 may be pressurized or

- - heated by a suitable fan/heater 76; hot pressurized air would be potentially useful. A remote monitor 80 could be. used to display an image of the section of vehicle 70 of interest. It is felt at this writing (and this applies also to the copending applications) that the return cone angle of the individual retroreflective elements, be they beads or corner cubes, etc., in the large array of such elements used on Scotchlite, Reflexite or similar screens, contributes to the sensitivity of the system. This is particularly thought to be true in the off-axis viewing mode; in other words the present roughly 2 degree return cone angle of the glass beads used in Scotchlite 7610 or 7615 produces good results. However, even sharper results could be produced if a screen with, say, a 1 degree cone were available. It may be alternatively desirable to "de-tune" the system when one does not want to see certain effects, and this could be effected by using a screen with, say, a 5 degree return cone. For use on index changes having high frequency, the point source is extremely valuable. Where broad effects such as waves in glass are to be viewed, a larger source size is possible. Typical satisfactory point sources include half inch apertures over flash guns with a screen-to-light-source distance of 10 meters (30 ft.), halogen movie light bulbs but without the rear reflector as at the same distance, etc. Even smaller sources are available, but one reaches a limit of being unable to sufficiently illuminate the screen in order to see the effect with the eye. If a TV camera is used, it is of course possible to increase the sensitivity of the camera and therefore decrease the size of the source. The same is true with high speed photographic film. Generally speaking it has been found preferable to focus the camera on the retroreflective material screen, or somewhere between the screen and source of index change. It is also possible, as disclosed in the copending applications, to have an alternative grid (or other portion) based arrangement 90. This includes placing grid lines on the screen or making the screen out of retroreflective strips, grids or other periodic members. It can also be accomplished by projecting a grid 91 or other pattern as shown in Fig. 3B onto a screen 94 using a Renchi Ruling 96, and light source 98, and lens 100. As shown, distortions in medium 100 cause modulation 104 of the grid 92 on screen 94. These modulations are imaged by a TV camera 106 using a beam splitter 108. As disclosed in the copending

SUBSTITUTE SHEET applications, this allows grids to be easily changed rotated, dithered, etc. As noted previously, data may also be processed by determining grid line deviations (as a result of index change) , by comparing the returning grid images to standard images (e.g. by optical filtering) or the like. The returning image can be filtered to show changes only when deviation occurs.

In this particular aspect of the invention, examination is being made of the deviation in the surface curvature of a refractive medium, the amount of refractive medium, or the index of refraction of the medium itself. Aside from the experimental differences involved, the effect appears to be similar to that disclosed previously. On-axis illumination produces the most power, while off-axis illumination can provide desirable aspects of light/dark shading indicative of refractive surface or index contour variation.

In the above examples, the effect is seen by looking through the distorted index medium of the screen. In other words, both a "primary" (first pass that hits the screen) and a "secondary" (on the return pass through the medium) effect occurs.

The chief contributor seems to be the primary effect, i.e. the information concerning the disturbance needs to be present on the screen. In this case the possibility exists

UTE SHEET of creating a screen which directs the light to an imaging camera positioned such that the light never passes back through the medium in reaching the camera.

The glass inspection system of Figure 5 has been shown to be capable of detecting forming irregularities in windshields and waves both caused by the tin in the float glass process.

Figure 7 illustrates both reflective and transmissive (refractive) e_r_ood__ments of the invention wherein waves 120 on water in a tank are viewed. In the reflective eπixxJiment, light from a light source 122 is reflected off of waves 120 to a screen 124 and back to an observer 126. In the transmissive (refractive) embodiment, light from a light source 128 is passed through the water and a glass bottom 130 to a screen 132 and then back to an observer

134. Using the invention, wave data can be studied for its own sake, or the system used to view waves carrying ultrasonic image data produced by coherent beating of waves passing through an object with a reference wave (ultrasonic holography), for example.

Any suitable wavelength of light from ultraviolet to to infrared can be used, commensurate with the function of the retroreflective screen. The latter is typically composed of glass beads, but can be a myriad of minute corner cube reflectors for example. For visible light, t pical retroreflector size is 20-200 microns in width (diameter) , spaced closely adjacent to each other for maximum efficiency.

As noted previously, the best light source for producing these effects is a substantially point light source. For example at a screen distance of 20 meters (60 ft.), a 1/2" (1.2 cm) wide source works much better than a source 4" (10 cm) wide when viewing thermal gradients.

Citas de patentes
Patente citada Fecha de presentación Fecha de publicación Solicitante Título
US4310242 *1 Abr 198012 Ene 1982The United States Of America As Represented By The Secretary Of The Air ForceField test unit for windscreen optical evaluation
US4612797 *27 Jun 198423 Sep 1986Rockwell International CorporationLeak locating and mapping system and method
Otras citas
Referencia
1 *See also references of EP0267956A1
Citada por
Patente citante Fecha de presentación Fecha de publicación Solicitante Título
EP0449573A3 *26 Mar 199113 Ene 1993Tokyo Gas Co., Ltd.Gas detection device
EP2803972A4 *28 Dic 201215 Jul 2015Sumitomo Chemical CoGreen honeycom molding defect examination method, green honeycomb structure manufacturing method, and green honeycomb molding defect examination device
US5168322 *19 Ago 19911 Dic 1992Diffracto Ltd.Surface inspection using retro-reflective light field
US5206700 *26 Sep 199127 Abr 1993Diffracto, Ltd.Methods and apparatus for retroreflective surface inspection and distortion measurement
US70235423 Abr 20024 Abr 20063M Innovative Properties CompanyImaging method and apparatus
Clasificaciones
Clasificación internacionalG01N21/41, G01M3/38, G01F1/66, G01B11/16
Clasificación cooperativaG01M3/38, G01N21/41, G01N2021/1765, G01B11/16, G01F1/661, G01N2021/416
Clasificación europeaG01N21/41, G01F1/66A, G01M3/38, G01B11/16
Eventos legales
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