FIBER OPTIC CURVATURE SENSOR

Abstract: The device according to the present invention includes an optical sensing device including first and second lightguides positioned side by side, and preferably covered as a unit with a layer of transmissive material, wherein the lightguides are adapted to detect or sense the presence, location, identity and shape of external media through modulation of the intensity of light coupled from one lightguide to the other through the transmissive material.

Description: FIBER OPTIC CURVATURE SENSOR Field of Invention This invention relates to fiber optic devices, and in particular optically sensing and measuring contact and shape, and classifying their properties. Background of the Invention Prior art optical contact and shape sensor methods include detecting contact pressures by means of frustration of internal reflection, which can take on many forms. Prior art contact sensors have been used to produce pressure contact images by having an external object deform a solid sheet into contact with a clear optical layer, the surface of the layer being illuminated by light which it reflects internally onto a camera. The contacting solid or intermediate sheet replaces a covering layer of air in a light guiding structure with the surface thereon, so that internal reflection at the point of contact is eliminated. In all cases, solids have a higher index than air, so even clear solids will tend to frustrate the reflections at the point of contact. The images collected by the camera or other vision system form pressure or contact maps that can be used for tactile sensing or object recognition. It is also known in the prior art that transmission of light through a fiber may be frustrated by micro bending, or overbending, whereby the fiber is bent with a curvature sufficient to cause some of the higher modes within the fiber to escape through the cladding because they strike the cladding at an angle exceeding the conditions for total internal reflection. An example of a microbending sensor is given in (Hastings, M.C. et al., "Evaluation of special communications grade fibers in interferometric and microbend sensors for measurements with ambient temperature fluctuations," SPIE Vol. 1795, Fiber Optic and Laser Sensors X, pp. 227- 235, 1992.) Microbending sensors, like the one indicated above, often use a shaped platen to impress multiple bends in a single fiber, thereby increasing the change in light throughput when pressure is applied. Sensors that detect or measure the extent of contact of a liquid are also frequently based on frustration of total internal reflection. Prior art liquid level sensors include single point detectors that can detect presence or absence of liquid at a discrete point, and continuous sensors that measure the spatially continuous height of a liquid. Examples of prior art optical liquid level sensors include US Patent 4,038,650 to Evans, US Patent 4,353,252 to Jeans, US Patent 4,788,444 to Williams, US Patent 4,039,845 to Oberhansli, US Patent 4,311 ,048 to Merz, US Patent 4,745,293 to Christensen, US Patent 3,448,616 to Wostl, US Patent 4,880,971 to Danisch, US Patent 5362971 McMahon, and WIPO 86/03832 to Bellhouse. Both Evans '650 and Jeans '252 describe point detectors that rely on frustration. Williams '444 and Oberhansli '845 describe point detectors wherein a similar frustration occurs within the wall of a containment. In the case of Oberhansli, the containment is the optical probe; Williams transfers the measurement to the wall of a clear container holding the liquid. Merz '048 uses a cylindrical rod with circumferential V grooves to obtain a quasi- spatially continuous measurement based on frustration at successive V grooves. A similar approach is taken by Christensen '293, except that non-circular V's comprise a grating, with V spacing corresponding to wavelength of the light. Successive mode extinction is used by Wostl '616 to achieve spatially continuous measurement using a tapered optical rod. Danisch '971 uses a multi-layered probe to achieve spatially continuous measurement independent of index of refraction of the liquid surrounding a smooth probe. Bellhouse 86/03832 uses a loop of optical fiber directly immersed in a liquid, the internal reflections being partly frustrated by presence of liquid where there would ordinarily be air. A loop or loops, small enough in radius to cause egress of light, are used to increase the dependence of internal reflection on external media. Loops of this sort are best achieved with plastic optical fiber, which can be formed into tight curves without cracking. Maximum frustration in looped sensors of this sort is achieved by removing or disturbing the clear cladding layer on the fibers, such as by roughening with sandpaper. A similar looped approach is taken by McMahon '971. McMahon quantifies the performance of loops of various diameters from 1/8 to over 3/8 inches in diameter. Water produces a loss of from 10 to 20 percent of the throughput in air, while gasoline produces a loss of approximately 45 percent. Examples of prior art for fiber optic shape sensing is given in Danisch patents: US 5,321 ,257, US 5,633,494, WIPO 0,702,780, and PCT WO 98/41815; and publications: Danisch, L.A, "Laminated BEAM loops," SPIE Vol. 2839, Fiber Optic and Laser sensors XIV, 12 pp., 1996; Danisch, L.A., Englehart, K., and Trivett, T., "Spatially continuous six degree of freedom position and orientation sensor," Fiber Optic and Laser Sensors and Applications, SPIE Conf. 3541 A, Boston, MA, 1998; and Danisch, L.A., "Smartmove Human Machine Interface," Volume 1 of report to Canadian Space Agency, Project 9F028-7-7153/01 -SW, 102 pp. + appendix, Dec. 13, 1998. In this prior art, the sensors report single degree of freedom curvature or complete shape using bend sensors alone, or an array of bend and twist sensors, respectively. In (Danisch, LA., "Smartmove Human Machine Interface," Volume 1 of report to Canadian Space Agency, Project 9F028-7 -7153/01 -SW, 102 pp. + appendix, Dec. 13, 1998) sensor arrays are described which report complete three dimensional shapes of an object by measuring bend and twist along a continuous flexure. In Danisch, '257, '494, 780, and '815, sensors are described which report monotonic (all positive or negative) curvature as a single valued output signal. The described sensors either have short sensing lengths, thereby ensuring monotonicity, or are long but used only in situations where monotonic curvature predominates. The prior art does not describe sensors designed to resolve or discriminate shape on the basis of a single output number, other than to correlate a single number with a net change in angle over a long sensor length. This "averaging" is described in Danisch, '494, col. 19, lines 9-14: "Nevertheless, spaced emission surfaces are still an advantage for many sensors, as they can be used to sense average curvature over a greater axial length of the fiber. This can eliminate or reduce undesirable effects from large local changes in curvature, for instance due to the presence of a foreign body under the fiber." Similar "averaging" is used in various other commercial devices to measure net angular changes. Examples include Penny and Giles goniometers and Virtual Technologies Inc. instrumented gloves, both of which use resistive bend sensors. These sensors report net angular change at the ends of a long flexural sensor, without regard to the intervening shape of the sensor. New shape sensing art introduced in the description of the present invention includes single and double fiber sensor structures capable of generating a distinctive, yet single-valued output which can be used to determine the class of shape applied. Classes of shape include curvature parameters such as monotonic, inflected, number of inflections, local magnitudes beyond high or low limits, spatial frequency content, and number of peaks of a given spatial frequency content. The new art is distinguished from the above "averaging" technique, because it does respond to the intervening shape. Other new shape sensing art based on double fiber structures similar to those used for shape classification enables improved measurement of curvature at distinct locations, including wavelength-encoded arrays of sensors that can be used to produce 3D measurements like those described in Danisch, 9F028-7-7153/01 -SW, cited earlier in this document, but with as few as two fibers. Summary of the Invention This invention comprises sensors made from single and multiple lightguides used as modulators, wherein the intensity of light passing through the lightguide(s) is changed (modulated) by a) external influences that change the shape of the lightguide(s), or b) external influences that change the optical media surrounding lightguide(s) shaped to be sensitive to contact with gases, vapors, liquids, or solids; without necessarily further influencing the shape of the lightguide. It can be advantageous to sense curvature or shape of a surface. This can be useful in sensing disturbances to civil structures, movement between parts, impacted shape of an automobile for purposes of deploying protection devices, or as a means of inputting information to a computer. For occupant or pedestrian protection device deployment (safety system deployment), such as air bag deployment, the deployment decision is made by an on board computer that must receive input on the type of shape impacting. For instance, a very sharp shape, as from a utility pole, which might cut through the metal without activating an accelerometer used to detect impact, is to be distinguished from a very broad shape that would be detected by the accelerometer. Other shapes such as multiple poles, or inflected and non- inflected shapes must often also be classified as part of a deployment decision. It is particularly important to detect shape of impact at the side of the car, where there is little material between the occupants and the colliding object. For low cost shape sensing, such as for safety system deployment (e.g. air bag deployment), it is desirable to use the smallest number of sensors possible. This can be accomplished by classifying shapes with a small number of long, flexible sensors, each designed to detect a certain class or classes of shapes. The sensors are attached, for instance, next to each other along part of the side of the car, such as along a horizontal door beam. It is desired to obtain single-valued outputs from each sensor that can be interpreted individually to determine the class or classes reported by each sensor, and in concert to resolve the class of shape impacting and its rate of penetration. Particularly difficult classes to distinguish from each other are single and double sharp impacts (e.g. a utility pole vs. two small vertical pipes). A sensor that simply integrates the absolute value of curvature along its length will tend to report the double impact with the same output as a particularly severe single-object impact. This is undesirable, because the two events often require different deployment actions. Another difficult pair of cases to distinguish includes broad and sharp shapes, such as those resulting from a guard rail and a utility pole, respectively. It is also advantageous to know the position and weight of seat occupants in vehicles, for purposes of automated safety system deployment. It is further advantageous for this application to classify occupants by "configuration," such as "occupant is in an infant seat with sharp edges" or "occupant is of average weight, seated in the middle of the seat". Information on these parameters can be found by measuring curvature or aspects of curvature, over the seat area, or chosen portions of the seat area. It can also be advantageous to measure the presence, absence, and nature of media contacting a sensor structure. The same sensors used to make shape measurements can be made sensitive to media contact, by forming them into particular shapes that cause some of the light travelling through them to interact with the surrounding media. It has been determined that with looped plastic fibers 0.25 and 0.5 mm in diameter, if any clear covering layer is used to protect the loops from external media, the maximum loss of light throughput that can be expected in the presence of water is 33%, and in most cases it is in the 10-20% range. Typical coverings are clear epoxy or a sheet of curved material such as polyethylene or polyester. If an array of many looped sensors is built with such covering materials, small variations in the thickness and integrity of contact with the covering materials will cause the losses at each sensor to differ greatly, so that it is difficult to process the signals from the loops without a calibration table. However, frequent re-calibration is necessary because minor contamination of the coverings by dirty films or particulates will change the signal levels even more than the change due to liquid replacing air as the external medium. It is possible to build an array with collections of prisms or similar structures, but this increases its size, expense, and vulnerability to damage and contamination. It can be advantageous to use an array of sensors to determine contact over a surface or along a line, at discrete points. Such arrays can be used to measure height or presence of a liquid or contact of a solid. Such an array will be most useful if each element of the array produces a large change in signal due to contact, and only a minor change due to presence of contamination such as by films of oil, dirt, dust, or chemicals. Changes on the order of 90% due to contact will make it unnecessary to calibrate the array, the signals being essentially binary. Yet, even though contact will be determined by essentially binary information, readings of the low light throughput after contact can be used to infer the nature of the contact, such as whether it is from a liquid of high or low optical index of refraction. If a sensor experiences only a minor change due to contact, such as 20%, this drop in signal can be mimicked by a contaminant that also changes the signal by 20%, which can occur easily. This is to be contrasted to a sensor with a throughput which drops to 10% in the presence of water and to 5% in the presence of oil. 20% contamination would change these values to 8% and 4%, but they would still be quite useable to report that a) contact had occurred and b) the type of substance in contact. The present invention enables very high modulation of light throughput due to contact with liquids, resulting in readings that are minimally influenced by layers of contamination. For most applications, whether for shape or contact sensing, it will be necessary to have the elements of the array protected from the surrounding media. This is especially true if plastic fibers are used for the array. For looped arrays, plastic fibers are the most useful, because they can retain a sharp bend without propagating micro-cracks and eventually failing from a condition known as "static fatigue" in glass fibers. However, plastic fibers are quite vulnerable to damage from chemicals, such as organic solvents, and require coverings, especially if they are abraded to expose the core and increase coupling to the external media. Unfortunately, clear coverings on individual loops and many other optical structures tend to defeat the measurement of external media. Because the coverings are of high optical index of refraction, they will act as frustrators, so that contacting materials will impart little additional change in throughput. Coverings that do not contact the fibers closely will also defeat the purpose of the sensor, because internal reflections will be maintained due to air between the covering and the protective layer. The coupling region is preferably covered with a lenticular layer, although other suitable materials may be used. The choice of optical fibers as a sensing means imparts qualities of safety and freedom from electrical interference, both due to the absence of electrical conductors within the sensing probe. It also makes possible very small and flexible sensing structures. The present invention benefits from the use of loops or bends in optical fibers as optical sensors, yet overcomes the disadvantages of prior art sensing loops. A particular advantage is the virtually complete modulation of the coupled light by the presence of liquids and solids, or by induced curvature, even though the device includes a protective coating. This makes the device relatively insensitive to the presence of contaminants on its surface. Contaminants cannot penetrate through the coating to the fibers, and have minimal effect on the measured values. As such, various embodiments of the invention described herein use optical fibers or other light guides to achieve: a) Detection of a liquid or solid contacting a sensing element with one bend that includes a clear protective layer; b) Discrimination of the type of liquid contacting the element; c) Measurement of liquid height with multiple elements or multiple bends; d) Measurement of curvature at a single bend; e) Discrimination of single from multiple shapes when multiple bends are applied; Accordingly, one embodiment of the present invention is to provide an optical sensing device comprising a pair of optical fibers where the fibers are positioned side by side, and covered, as a unit, by a layer of optically transparent material having a convex arcuate outer surface. Another important aspect of the present invention is the exploitation of the shapes of paired loops or bends to impart an optimal shape to a clear protective coating that couples the loops or bends optically. The coating has a shape determined by the loops or bends and the flow characteristics of the coating material during its cure cycle. Another important aspect of the present invention is the exploitation of the shapes of fibers laid side by side to impart an optimal shape to a clear protective coating that couples the fibers optically when they are bent. The coating has a shape determined by the fibers and the flow characteristics of the coating material. Further aspects of the present invention include providing a sensor means that: a) can be formed into small individual point sensors or a thin, quasi-spatially- continuous array; b) does not expose the fibers directly to the media to be measured; c) is capable of discriminating water from hydrocarbons; d) is capable of detecting and measuring extent of contact with solids; e) can be used to measure curvature and classify multiple curvatures to classify imposed shape. f) if desired, can have an optical output of zero when not curved. g) can be manufactured and instrumented at low cost. Accordingly, it is another aspect of the present invention to provide an optical sensing device adaptable to detect or sense the presence, location and identity of external media. Accordingly, it is another aspect of the present invention to provide a means of forming a single point sensor or an array of these sensors from fibers that have been looped or bent and covered with a layer or layers of durable material, and yet provide maximum modulation (90% or more) when exposed to contact by liquids and solids. High modulation is desirable in achieving a liquid sensor that is able to be used to discriminate between different substances, such as a liquid and a gas, or between different liquids, especially in the presence of contaminating materials. Accordingly, it is another aspect of the present invention to form sensors between fibers of a fiber optic ribbon cable, at desired lateral and axial locations along the cable, so that pressure or imposed shape at the sensor locations will generate a signal due to curvature of the cable, associated with the location of the sensor. Accordingly, it is a further aspect of the present invention to provide a sensing strip with one or more fibers or other lightguides, so that impressed shapes will generate signal values from the sensing strip indicative of the class of shape impressed, based on combinations of curvatures contained in the shape class. It is still a further aspect to accomplish any of the above without use of special preformed optical shapes such as prisms or grooves, but rather to rely on the natural shapes of the loops or bends, covered with materials that do not require special forming processes, yet have a shape that produces the desired optical response. This also eliminates the need to connect fibers to optical elements such as lenses or prisms, thereby simplifying the construction process and increasing the reliability of the instrument. It is still a further aspect of the present invention to be able to construct a sensor array without requiring special alignment fixtures or molds to hold the fibers in place during and after construction. It is still a further aspect of the invention to form flat sensor strips, that can be applied to flat or gently curved surfaces and used to sense or classify shapes when impressed upon the surface, or strips that can be curved at desired locations to activate a contact sensing capability at said locations. It is still another aspect of the present invention to provide an inexpensive optical sensor device capable for use as a multi-use sensor, such as a single sensor construction that can be used to sense liquid level, pressure, and shape. According to one embodiment of the present invention, there is provided an optical sensing device comprising a first optical lightguide; a second optical lightguide with a portion of its length parallel to and in close proximity to the first lightguide to form a coupling region; the first and second lightguides being covered within the coupling region; and wherein, light is coupled from the first lightguide to the second lightguide, when the lightguides are curved out of their plane within the coupling region. Desirably, the above cover for the coupling region is formed by a lens layer of optically transmissive material having a convex, arcuate outer surface. In another aspect according to the above, the lightguides are mounted in a surface to be deformed by imposed pressures or shapes for purposes of determining classes and growth of impacted shapes. According to a further embodiment, the first and second lightguides are modified for enhanced coupling, by abrasion, chemical treatment, heat forming, or notching, to lose and collect light in adjacent surface areas facing away from the plane of the lightguides in the coupling regions. In this embodiment, coupling may be made to occur for both straight and curved lightguides. According to a further embodiment, used when shape, rather than contact with external media, is to be measured, coupling may be further enhanced by addition of a reflective layer surmounting the lens layer. A further embodiment includes means for injecting light into the first lightguide, and means for detecting the intensity of light coupled into the second lightguide. Further, according to the above including a means for injecting light into the first lightguide, means for detecting the intensity of light coupled into the second lightguide, and means for detecting the intensity of light carried through the first lightguide. According to another alternative embodiment, the lens layer is formed on only the side of the plane of the lightguides containing the loss and collection areas, thereby enabling coupling only for curvatures of the lightguides which impose convex curvature on the lens layer. Preferably, according any of the above embodiments, the transparent material comprises a synthetic resin, a heat dissolvable material or a chemically removable material. According to another aspect of the present invention, the first and second lightguides are formed into curves out of the plane of the lightguides, within the coupling region. In another alternative embodiment, there is provided a pressure or shape measuring and classifying sensor as described above, wherein the first and second lightguides are mounted on a surface to be deformed by imposed pressures or shapes. According to another aspect of the present invention there is provided a pressure or shape measuring and classifying sensor wherein the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that is maximal for only a single inflected shape and is attenuated when more than a single inflected shape is imposed. Desirably, the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that is maximal for shapes with large curvatures and minimal for shapes with minimal curvature. According to another embodiment of the above pressure or shape measuring and classifying sensor, the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that decreases for noninflected shapes and increases for inflected shapes, or to produce coupled light intensity that is minimal for inflected shapes and maximal for noninflected shapes. According to various alternative embodiments described above, there is provided a pressure or shape classifying sensor comprising a first or second lightguide wherein the intensity of light that has passed through the lightguide is measured to classify the shape imposed on said lightguide according to the number of inflected curves, polarity of curvature, and magnitude of curvature. In a further alternative embodiment according to the present invention there is provided a pressure or shape measuring and classifying sensor comprising a first plurality of sensors (as described in an above alternative embodiment), exposed to a distribution of curvature within an extent; and a second plurality of sensors (as described in an above alternative embodiment), exposed to a distribution of curvature within the extent; wherein the measurements of a pressure or shape distribution by the sensors are analyzed singly and in combination to classify the distribution of curvature within the extent according to absolute value, polarity, number of inflections, number of peaks, spatial frequency content, and location within the extent, and to measure the time progress of the classifications. Desirably, the above may be used for determining classes and growth of impacted shapes in vehicles for purposes of safety system deployment. Preferably, the above sensor may be used for determining occupant position and weight in vehicles for purposes of protection activation. According to another alternative embodiment of the present invention, there is provided a pressure or shape sensing array comprising sensors with coupling regions as described in any of the above embodiments, distributed over an area within which pressure or shape is to be measured at locations, wherein the sensor coupling regions are located to respond uniquely to pressure or shape at said locations and wherein the overall pressure or shape is inferred from the individual sensor measurements. Preferably, the above sensor array comprises electrical conductors instead of lightguides, the coupling regions comprise electric coupling regions wherein coupling is modulated by bending, and the bending is determined by measuring electric current or voltage resulting from the coupling. Desirably, the above sensors are formed from adjacent fiber pairs of a fiber optic ribbon cable, wherein each coupling region occupies a known location along the axial extent of the cable. According to another alternative embodiment of the present invention, the sensor is preferably located between first and second mechanical layers, said mechanical layers containing structures capable of bending the sensors when pressure is applied or shape is imposed through bending. According to any of the above alternative embodiments, there is provided a media contact or deformation measurement sensor wherein the combined loss and coupling properties of coupling regions modulate the light flux passing from one fiber to another across the coupling regions, wherein the properties of the coupling regions may be chosen to enhance modulation by contact with liquid, or by imposed pressure, bending, or shape. According to an alternative embodiment of the present invention, there is provided a liquid or solid contact measurement sensor wherein the coupling regions are preformed into curves that couple light maximally when surrounded by a medium of low index of refraction and which couple light minimally when surrounded by a medium of high index of refraction. Desirably, the above sensor is one in which a flexible surrounding material containing air at atmospheric pressure within is deflected by pressure from a liquid or solid medium without, to touch the curved coupling regions and produce changes in the measured intensity of light indicative of contact. According to another embodiment, there is provided a liquid or solid contact measurement sensor comprising a sensor with coupling regions preformed into curves along its extent, each curve of which couples light maximally when surrounded by a medium of low index of refraction and which couples light minimally when surrounded by a medium of high index of refraction. According to any of the above alternative embodiments, the sensors may include a planar support member having an edge, and where the coupling regions may extend over the edge or may be spaced apart along and extend over the edge. In yet a further embodiment a liquid or solid contact measurement device as above, the coupling region is preformed into a curve with its apex exposed at the end of a tube covering the device. Desirably, the above liquid contact measurement devices measure the intensity of coupled light when the device is immersed in liquid indicating the index of refraction of the liquid or level and composition of layered liquids. According to another embodiment, there is provided a liquid or solid contact measurement sensor as described above including an array with spaced sensors, and motive means for changing the liquid or solid level with respect to the sensor array by a known displacement up to one intersensor spacing, the array measurement and said displacement being used to determine liquid or solid height or composition along a continuum. In an alternative embodiment, there is provided a method of sensing a pressure or shape comprising the steps of providing a first optical lightguide, providing a second optical lightguide with a portion of its length parallel to and in close proximity to the first lightguide within a coupling region, covering the first and second lightguides within the coupling region, as a unit, by a lens layer of optically transmissive material having a convex, arcuate outer surface, transmitting light from a light source through the first optical lightguide, measuring the intensity of light coupled to the second lightguide through the lens layer, by measuring its intensity at the end of the second lightguide toward which said coupled light is directed, as a means of measuring curvatures within the coupling region. In another alternative embodiment there is provided a method of sensing liquid or solid contact comprising the steps of providing a first optical lightguide, providing a second optical lightguide with a portion of its length parallel to and in close proximity to the first lightguide within a coupling region, covering the first and second lightguides within the coupling region, as a unit, by a lens layer of optically transmissive material having a convex, arcuate outer surface, forming the coupling region into at least a single curve, transmitting light from a light source through the first optical lightguide, measuring the intensity of light coupled to the second lightguide through the lens layer, by measuring its intensity at the end of the second lightguide toward which the coupled light is directed, as a means of measuring the contact of liquid or solid and the index of refraction of the liquid or solid. In a further alternative embodiment, there is provided an optical sensing device comprising an optical lightguide, an actuation operable device associated with the optical lightguide, wherein the optical lightguide when deformed forms a coupling region adapted to transmit light along its length when the lightguide is curved out of its plane to the actuation device. Desirably, the above device includes means for injecting light into the lightguide, and means for detecting the intensity of light coupled into the lightguide. Further, the above device is preferably provided with a cover for the coupling region formed by a lens layer of optically transmissive material having a convex, arcuate outer surface. According to another aspect of the present invention, the above lightguide may be formed into curves out of the plane of the lightguide, within the coupling region. Desirably, the above lightguide may be mounted on a surface to be deformed by imposed pressures or shapes. According to an alterative embodiment according to the above embodiment, the device is provided for determining classes and growth of impacted shapes in vehicles for purposes of actuating a safety system actuation device. Desirably, the device further provides for determining occupant position and weight in vehicles for purposes of safety system deployment According to another alternative embodiment, the device may be used for determining classes and growth of impacted shapes along gaskets and seals. Preferably, the above lightguide is mounted in a surface to be deformed by imposed pressures or shapes for purposes of determining classes and growth of impacted shapes. When used to measure pressure, bending, and shape, when it is not desired to have interactions with external media such as liquid contact, the coupling regions of the device preferably include a reflective layer surmounting the lenticular region, to increase the light coupled across the coupling zone and extend the range of curvatures and pressures measurable with the device. According to another preferred embodiment, the device may be used to sense shape and liquid contact using coupling regions formed with lightguides of zero curvature, by enhancing the loss of light from lightguides in the coupling regions through abrasion, heat forming, notching, or chemical treatment. For shape and bend sensing alone, coupling is optimized by such loss enhancement, combined with the addition of the above reflective layer. According to another preferred embodiment, the coupling regions in the device may each be made responsive to a particular wavelength or band of wavelengths of light, through adding wavelength filtering media to the lenticular medium or reflective layer of each coupling region. BRIEF DESCRIPTION OF THE DRAWINGS The invention will now be described, with reference to the drawings. FIGURE 1 is a side view of an optical fiber curved sufficiently to emit light, emitting light. FIGURE 2 is an edge view of the same fiber in Figure 1. FIGURE 3 is a side view of the fiber of Figure 1 , receiving light. FIGURE 4 is an edge view of the fiber of figure 3, receiving light. FIGURE 5 is a graph plotting the optical throughput of a fiber as in figures 1 - 4, when bent at various curvatures. FIGURE 6 is a perspective view of two fibers coupled by a lenticular layer along a coupling region, including options for enhanced coupling comprising a reflective layer and enhanced loss treatment. FIGURE 7 is a plan view of the fibers of Figure 6, straightened and including a light source and receiver, but without the options for enhanced coupling. FIGURE 8 is a cross section through the two fibers on the line A-A of Figure 7. FIGURE 9 is an edge view of the fibers as in Figure 7, bent within the coupling region. FIGURE 10 is a perspective transparent view of curved fibers as in figure 9, including a lenticular layer along a coupling region. FIGURE 11 is an edge view of the fibers of figure 10, showing light emitted from one fiber, reflecting internally within the lenticular layer, and entering the second fiber. FIGURE 12 is a cross section on the line B-B of Figure 10, showing the coupling of light from fiber to fiber within the lenticular layer. FIGURE 13 is a graph of the optical intensity throughput for light injected into one fiber of a coupled pair as in figure 10, for varying amounts of curvature of the structure. FIGURE 14 is a perspective view of two fibers coupled by a lenticular layer, treated to have enhanced coupling areas along their upper surfaces, to enhance their ability to couple light from one fiber to another at lower curvatures than untreated fibers. FIGURE 15 is a cross section of the line C-C of Figure 14. Figure 15a is a cross section as in Figure 15, but with the addition of a reflective layer surmounting the lenticular layer. FIGURE 16 is a perspective view of a coupled fiber structure as in Figure 15, but with multiple enhanced coupling areas applied along the upper surface, for piecewise continuous coupling between the two fibers. FIGURE 17 is a schematic view representing the fibers as in Figure 16, with a longer coupling area indicated by the region containing overlapped lines. FIGURE 18 is a schematic view representing the same two fibers of figure 17, bent in a single inflected shape within the coupling area. FIGURE 19 is a schematic view representing the same two fibers of figure 17, but with two inflected shapes applied within the coupling area. FIGURE 20 is a graph showing total throughput vs. number of separate curves, for a mathematical model of a coupled fiber structure as in Figure 17, for different attenuations at each curve, and a normalized throughput of 1.0 for each curve, before attenuation is applied to each coupled throughput. FIGURE 21 is a schematic view of a coupled fiber sensor as in Figure 17, with multiple sinuations that can be used to sense the level of a liquid or amount of contact with a solid surface. The fibers include a turnaround loop so that light source and detector may be co-located. FIGURE 22 is a schematic view of a single fiber sensor with a light source at one end and a light intensity detector at the other end. FIGURE 23 is a schematic view of a fiber sensor with two parallel runs of fiber coupled by a loop, so that source and detector are co-located and the net throughput is a product of the throughput of individual purposely imposed enhanced coupling areas along the fibers and curvatures imposed on the fibers by an external force, said enhanced coupling areas optionally having different characteristics on each fiber. FIGURE 24 is a schematic view of a coupled fiber structure with one fiber extended, so that throughputs may be measured for light that traverses one fiber from beginning to end, and for light that traverses in lenticularly coupled fashion from one source on one fiber to a detector on the other fiber. Figure 25 is a schematic view of a coupled fiber structure of Figure 24, with loops incorporated so that all sources and detectors may be co-located and more than one fiber run traverses the sensor area, each run being coupled by a loop to the next run, so that detected signals are the product of multiple runs. FIGURE 26 is a perspective view of a lenticularly coupled sensor in the end of tubing. FIGURE 27 is an edge view of the sensor of Figure 26, with the transmitting fiber on the left. FIGURE 28 is an edge view of the sensor of Figure 27, with the transmitting fiber on the right. FIGURE 29 is a perspective view of two elements of an array of lenticularly coupled sensors, built on the edge of a thin band of steel. FIGURE 30 is a simplified view of a complete array of four paired loops or bends attached to an interface box. FIGURE 31 is a simplified view of an alternative embodiment of the present invention including a complete array of four paired loops attached to an interface box, arranged in a standpipe to measure liquid height. FIGURE 32 is a pressure sensor array formed from fiber optic ribbon cable, with coupling zones formed at discrete locations between fiber pairs by forming a clear lenticular structure at each location. FIGURE 33 illustrates a coupled fiber arrangement with mirrored ends. FIGURE 34 illustrates a mirror ended arrangement having multiple zones. FIGURE 35 illustrates a mirror ended arrangement having multiple zones, the zones angled. Having thus generally described the invention, reference will now be made to the accompanying drawings illustrating preferred embodiments. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS As illustrated in Figures 1 and 2, a fiber 10 curved sufficiently, will lose light along its periphery because some of the higher modes are unable to reflect internally within the fiber core. For simplicity, a thin cladding layer of low index of refraction, typically surrounding the core of all step index fibers, is not shown in the figures unless otherwise indicated. The cladding layer 24 is used to maintain internal reflection within a straight fiber even if it comes into contact with solids or liquids. If there is no such contact, air will serve as a low index of refraction material to maintain internal reflections. Whether or not there is a cladding layer, a fiber curved below its minimum bend radius will begin to lose light. Example rays of light YY are shown leaving the fiber 10 where it is curved. Although the term "fiber" for "fiber optic" is used throughout the description, it is meant to apply generically to lightguides of various types, including clad or unclad bars of clear plastic or glass, of round, rectangular, or other cross section, capable of guiding light within the bar due to internal reflection. Figure 2 shows the fiber 10 of Figure 1 from the edge. Example rays of light YY are seen to be emitted not only within the plane of the loop, but within a cone of angles bisected by the plane of the loop. As shown in Figure 3, a fiber 10 bent sufficiently to lose light is also capable of receiving light within the same range of angles that it can be emitted. Example rays YY are shown entering the fiber 10 where it is curved. Figure 4 shows the fiber 10 of Figure 3 from the edge. Example rays of light YY are seen to be received not only within the plane of the loop, but within a cone of angles bisected by the plane of the loop. After entering the receiving fiber, the light will continue to propagate down the fiber 10 within the cone of angles determined by the index of refraction of the core and that of its cladding 24, or other surrounding medium. Figure 5 is a curve illustrating the loss of light throughput for a 0.25 mm diameter multimode step index plastic optical fiber 10 bent in a 180 degree circular curve (a "C" shape) at various radii in air. Throughout this description, throughput is defined as intensity of light collected at the output of an optical system under conditions of constant light input. In this figure, unattenuated throughput is represented by a value of 1.0. The fiber 10 begins losing light at a radius of approximately 5 mm, and continues to lose more and more light as the radius decreases. Larger fibers begin to lose light at larger radii. For instance, a 0.5 mm fiber will begin to lose light at a 10 mm radius, a 1.0 mm fiber at 20 mm, etc. A similar graph could be generated showing the receptivity of a fiber to external light along a curved section, with receptivity to a wider range of angles corresponding to smaller radii of curvature. Figure 6 illustrates a dual fiber 12, 14 sensor structure. The fibers are parallel and in close proximity within a "sensing zone" or "coupling region" 20 that is covered by a lenticular layer 22 of clear material. The lenticular layer 22 may be applied to the full length of the overlapped fibers 12 and 14, or to a subset of the length. For convenience or to provide mechanical protection, the same material may coat the non-overlapped fibers. Figure 6 shows the core material 8 of the fibers, having a high index of refraction, and the cladding layer 24, having a lower index of refraction. It is also possible to omit the cladding layer if the cores have little contact with materials of high index of refraction, such as by using acrylic rods extending in air. Also shown are loss treatments 113 which are optionally used to increase the egress and ingress of light through the core-cladding interface, and a reflective layer 116 which may be used to further enhance coupling and increase the range of operation of the sensor when coupling to external media is not required. These optional coupling enhancements are discussed further in association with Figures 15, 32 and 33. Figure 7 shows the fibers and coupling region of Figure 6 in plan view, with the fibers straightened and with a light source 16 and light receiver 18, coupled to lightguides 12 and 14. For simplicity, the cladding layer 24 and the optional structures 113 and 116 of Figure 6 are not shown. Figure 8 is a cross section through the overlapped portion of the sensor structure within the coupling zone 20. By way of example, in this figure, the core 8 and cladding 24 on the fibers 12, 14 is shown. The lenticular layer 22 is shown as an oval shape surrounding the fibers. The following conditions apply to the lenticular layer: a) It can be of any shape capable of reflecting light from one fiber to the other along lines defined by the emission and receiving characteristics of fibers curved below their minimum radii of curvature or with cladding modified to enhance egress and ingress of light. Typical cross section shapes are convex as shown or flat. Even concave shapes will serve. b) It can be on one side of the fibers or both. If it is on one side, the sensor will only function when it is curved convexly on that side. c) It can be of any index of refraction higher than that of air. Preferably, it will have an index in the 1.5 or higher range, typical of most materials capable of coating fibers. However, the sensor will function when lower index materials are used, such as silicones in the 1.4 -1.5 range of index of refraction. d) It should have sufficient clarity to transmit light the short distance from one fiber to the other, but need not be of exceptional clarity. Ordinary epoxies, urethanes, casein resins and other coatings will function well for the short path encountered by light traveling from one fiber to the other. e) It may be covered by a layer of other material of low index of refraction, or by a purely reflective material such as a metal film, for protective purposes or for cases where the sensor is to be used primarily as a means of sensing shape, with minimum coupling desired to external media and maximum coupling desired from fiber to fiber. The fibers within a lenticular layer 22 should be in close proximity, or the lenticular layer 22 made thicker to enable light to couple at the necessary angles for propagation when the fibers are bent. In most embodiments, the fibers will be touching in the overlapped regions, but can be several millimeters apart if the lenticular layer 22 is thicker. Preferred methods for forming a lenticular layer 22 on adjacent parallel fibers include: a) Spreading a synthetic light transmitting resin on the fibers with a spatula to fill the grooved space between the fibers. The resin will take on a flat or crowned cross section due to surface tension effects while curing. b) Applying a continuous bead of synthetic light transmitting resin on the fibers through a syringe tip, with size of the bead controlled so that when it is curing, it will fill the grooved space between the fibers, taking on a crowned shape in cross section. c) Applying an excess of synthetic light transmitting resin on the fibers, and wiping it off with gloved fingers or flexible spatulas so that when it is curing, it will fill the grooved space between the fibers, taking on a crowned shape in cross section. d) Any of the above, where the grooved space on both sides is covered with resin simultaneously, the fibers being suspended in air. e) Any of the above, where the fibers are held together with temporary adhesive while the resin is being applied. A reflective layer may be added by vacuum or chemical deposition of metal vapour on the lenticular region after it is formed, or by adhesion of metal foil or other reflective material such as reflective beads, prisms, or colloidal suspensions. The lenticular shape of the coupling material is also a preferred shape when used with a reflective material. A reflective layer directly on the fibers would prevent coupling. The lenticular shape allows space for light to exit one fiber, and then enter the other fiber. For straight lightguides with intact cladding, as shown in Figure 7, there is negligible coupling of light from one fiber to the other in the coupling zone, so there is no signal detected by the light receiver. In the present invention, evanescent coupling between adjacent fibers, which arises from photons having no finite boundaries according to the wave theory of light, is not considered to be a significant contributor to any of the coupled light. Figure 9 shows the sensor structure of Figures 6 and 7, now in edge view, but with the sensing zone 20, covered by transparent material 22, bent in a 180 degree curve at a curvature where the untreated fibers are capable of emitting and receiving light. Figure 10 shows the sensor structure of Figure 9 in more detail, including the two curved portions of the fiber in close proximity to each other, and surrounded by the lenticular layer 22. Figure 11 shows the sensor structure of Figure 10 in edge view, including arrows indicating the paths followed by example rays leaving the emitting fiber, reflecting internally within the lenticular layer 22, and entering the receiving fiber. Figure 12 shows the sensor structure of Figures 10 and 11 in cross section, including arrows indicating the paths followed by example rays leaving the emitting fiber, reflecting internally within the lenticular layer 22, and entering the receiving fiber. In this figure the cladding layers are shown on the fibers. Figure 13 is a graph of the coupled throughput of the sensor structure of Figure 9, for a 180 degree, or "C" shaped curve, for different radii of the curve. For radii above the minimum bend radius of 5 mm, there is very little or zero throughput, whereas the throughput rises dramatically as the curvature (curvature is the inverse of radius of curvature) increases. Figures 14 and 15 illustrate a sensor structure including overlapping fibers surrounded by a lenticular layer 30, in a sensing zone 32. In this case, the fibers are treated to lose light along narrow strips by abrading or other methods described in patents by Danisch, US 5,321 ,257, US 5,633,494, and WIPO 0,702,780 to increase their ability to modulate throughput in response to bending. These treatments, shown in Figure 14 as short parallel lines 34 along fiber 26 and similar lines 36 along fiber 28, and on Figure 15 as striped regions in the core-cladding interface at the tops of the fibers also serve to couple light into the fiber, so serve as a means of "enhanced coupling" between the fibers even when they are straight or bent without violating the minimum bend radius. In this alternative embodiment, the treatment is applied to enable use of the sensing zone 32 at large radii of curvature. For instance, the structure used to generate the graph of Figure 13 has no throughput for radii above approximately 5 mm, but the same configuration with abraded zones as in the present figure begins to lose light for radii of 10 cm, and wider or deeper "enhanced coupling" zones can be applied to achieve coupling even for straight fibers. If the enhanced coupling zones are restricted to one side of the fiber, coupling will increase for bends that curve the enhanced coupling zones convexly, even for large radius bends, but coupling will normally be minimal or zero for bends in the other direction until microbending effects begin to take place (e.g. 5 mm radius for the fibers in this example). An exception to this can be created with fibers that have enhanced coupling zones with very high loss or where an optional reflective layer 116 is added above the lenticular layer, as shown in Figure 6 or Figure 15. Then, coupling may be nonzero even for straight fibers, and will decrease to zero when the enhanced coupling zones are increasingly concave. Given that loss strips may be applied in various lengths, spacings, and conformations given in Danisch '257, '494, and '780, including on one side or two sides, or circumferentially around the fibers, many throughput vs. curvature characteristics are possible. An example of bipolar enhanced coupling zones distributed along the fibers in quasi- continuous fashion is shown in Figure 16. The distribution is made quasi-continuous to prevent depletion of loss modes as described in Danisch '257, '494 and '780. It is also desirable to displace the collection zones 40 "downstream" (away from the light source) of the loss zones 42, because light loss occurs at angles directed away from the source, and collection is optimal for angles directed toward the source. A typical downstream displacement for 0.25 mm fibers is 0.5 to 1 mm. The embodiment shown in Figure 15a is similar to Figure 15, but shows a reflective layer surmounting the lenticular layer. Characteristics of coupled fiber structures with different types of enhanced coupling zones include: a) Monopolar: throughput responds equally to curvatures of either polarity. This can be achieved with untreated fibers beyond the minimum radius of curvature, or with fibers treated on both sides or circumferentially, within a larger range of radii. Monopolar sensors respond to the absolute value of curvature. b) Bipolar: throughput increases for one polarity of curvature, decreases or is unchanged for the other. This can be achieved with fibers treated heavily on one side and can be further enhanced by using a reflective layer over the lenticular layer. c) Nonuniform or nonlinear: throughput responds differently for different classes of curvature. For instance, the throughput of coupled fibers treated with enhanced coupling zones will respond with gradual changes to large radius bends, and will respond with increased sensitivity to bends within the range of radii where microbending effects predominate. d) Spatially varied: If enhanced coupling zones are applied with varied spacing and length, coupled fiber structures may be achieved that have zones of sensitivity and insensitivity along their lengths. Curvatures applied to the fibers may tend to miss the sensitive zones, or be poorly sampled by the sensitive zones, or not have any effect or minimal effect in zones that are purposely designed to be insensitive or minimally sensitive to curvature. All of the light coupled from one fiber to another in a coupled fiber sensor without the addition of a reflective layer, as in Figure 9 relies on internal reflection within the lenticular layer 22. Without internal reflection, which relies on the presence of a medium of low index of refraction compared to that of the lenticular layer 22, surrounding the lenticular layer 22, coupling will be reduced to a lesser value or to zero, depending on the index of the surrounding medium and its extent of contact with the curved portion of the fibers. The following are examples of measured throughput for various media surrounding lenticularly coupled loops with a radius of 1 mm, referenced to a normalized value of 1.0 for air: a) Air (index of 1.00): 1.0. b) Water (index of 1.33): 0.08 c) Motor oil (index of 1.43): 0.04 Many other hydrocarbons have indices in the 1.4 to 1.5 range, and produce results similar to that of motor oil, and always easily distinguished from those of water or air. When solids come in contact with a curved coupled fiber sensor, the coupled light is also frustrated, to a degree dictated by the contact surface area. The surface area of liquid contact also determines the throughput for a single loop, the throughput rising to a maximum for total contact. Figure 17 shows a coupled fiber structure in schematic form, with the fibers 12, 14 drawn as two parallel lines, overlapping within an oval shape 20 of exaggerated width, meant to represent the coupling region formed of transparent material 22. Figure 18 shows the fibers of Figure 17 with a curvature applied in the shape of an inflected curve 50. This may be thought of as the shape of a dent applied to the side of an automobile, or curves in a flexible coupled fiber pressure sensor caused by pressure from an object such as a finger, or could represent fibers that are held in constant curves so that liquid or solid contact may be sensed at the curves. The curves are said to be inflected because they include positive and negative values of curvature. The two polarities of curvature are illustrated schematically by upward convex arcs 53 representing negative curvature and downward convex arcs 55 representing positive curvature. In this example, the two positive curves have a net angular change of approximately 90 degrees each, and the negative curve has a net angular change of approximately -180 degrees. The algebraic sum of the net angular curvatures is zero. This is confirmed by the fibers entering and exiting the inflected curve in the same horizontal orientation. Figure 19 shows the fibers of Figure 17 with two inflected curves 52, 54 applied at different locations along the coupled portion of the fiber. Figure 20 depicts the calculated throughput of a sensor as shown in Figure 19, but with the number of inflected curves varying from one to five. It will be described in more detail below as the equations for throughput are derived. Figure 21 depicts a sensor as in Figure 17, but with multiple sinuations 58 preformed in the coupling region, which is indicated by the overlapped fibers within the sinuated oval shape representing the lenticular transparent material 22. It will be described in more detail below in the context of liquid sensing. It is presented here in association with Figure 19, as an example of a coupled fiber sensor with multiple sensing curves 58 and a non-sensing turnaround loop 60. In the case of Figure 19, the multiple curves result from a temporarily imposed shape. In Figure 21 they are permanently pre-formed to enable contact sensing of a liquid. We now address the issue of throughput for single and multiple curves along the fibers. First, we will consider a single fiber 12 like one of the fibers shown in Figure 17, but with source 16 and detector 18 connected to the two ends. Such a fiber is shown in Figure 22 and again in Figure 23. In Figure 23 a loop 60 is incorporated so that source and detector may be co-located, and two runs of fiber 13 and 15 coupled only by the loop 60, but exposed to the same imposed curves along their lengths, may be treated differently by means of purposely imposed enhanced loss zones of different constructions, so that each run contributes in a different way to the net throughput signal when curves or contacts are imposed on runs 13 and 15 simultaneously. The different treatment of the runs 13 and 15 is indicated schematically by different linestyles for each run. . Within a single fiber run or runs coupled only by a loop of the same fiber and with no other coupling means used, the net throughput is a product of the losses at each curve. If a fiber has n curves, each curve i in the fiber has a throughput Ei resulting from microbending or purposely imposed loss zones, and if Es is the net throughput of such a single fiber (normalized to unity for unattenuated throughput) , then (Eq. 1 ) Es = where the product [ is taken from the initial through the nth curve i. Thus, if 6 equal curves each of throughput 0.5 are applied, the net throughput Es = (Ei) n = 0.5 x 0.5 x 0.5 x 0.5 x 0.5 x 0.5 = 0.016. Three curves of throughput 0.5 result in Es= 0.125, or 8 times more throughput than 6 curves. The "6 curve" vs "3 curve" example is relevant to comparing the effects of a single dent to those of double dents, where each dent includes a positive and two negative curves of equal magnitude, and the coupling is monopolar (equal for any polarity of curvature). At first it might seem useful to have multiple dents produce less throughput than a single dent, but it must be remembered that in a single fiber sensor, reduction in throughput is a signal indicating increasing depth of a dent, so that multiple small dents will mimic a single large dent. This is the opposite effect to that desired for air bag or other safety system deployment, for which one may wish to ignore multiple small dents. However, a single fiber sensor may be useful in detecting sharp vs. broad dents. The former will produce more attenuation than the latter, due to the larger curvatures implied by sharp vs. broad dents. By varying the type and placement of loss zones, it is possible to create single fiber sensors that respond differently to different shapes. In the example above, the sensor responds with increasing attenuation to higher curvatures or more dents. If enhanced coupling zones of minor attenuation are applied to one side of the fiber, then a saturated response in throughput to bends of a given polarity can result. As shown in Danisch, US 5,633,494, and WIPO 0,702,780, a lightly treated (an imposed enhanced coupling zone with small attenuation) sensor fiber will exhibit a throughput that saturates at a high value for concave bends of the treated zone above a characteristic curvature, and which continues to decrease for increasing bends in the opposite, convex direction. If such a sensor is used to detect dents, it will have an accentuated response to bends in the convex direction, so that it can be used, for instance, to classify inflected dents from noninflected (monotonic) dents. This is done by applying the sensor so that noninflected dents cause convex curvature of the treated zones, thereby causing an increase in throughput that saturates, whereas inflected dents will cause a large net decrease in throughput due to the imposition of two concave curvatures with unsaturated decreasing throughput at the edges of a single convex curvature that saturates at a low value of increasing throughput. If the sensor is inverted so that noninflected curves cause a decrease in throughput, they will be sensed as a non-saturated decrease in throughput. Inflected dents will also cause a decrease in throughput, representing the product of one convex curve (large unsaturated decrease) response with two concave curve responses (small saturated increases). Sharp inflected dents will produce larger drops in throughput than broad inflected dents, since most broad inflected dents will have two concave edges that are below the saturation limit, and will have a net zero product, the net result of one small decrease and two small increases. Others may be made into sensors that have no treatment, in which case they will respond with attenuation that increases for sharper bends or more bends, without regard to polarity of curvature within the microbending range; or with loss zones on both sides, so that response also disregards polarity but is not restricted to the microbending range; or with loss zones on one side but such that response is bipolar (regards polarity of curvature) over a broad range of curvatures (as opposed to the bipolar saturated response described above). Treated fibers with a bipolar response may also be used to classify noninflected shapes from inflected shapes. Inflected shapes that begin and end with zero curvature have a net curvature of zero regardless of the curvatures within the shape, so will be "invisible" to a bipolar sensor. In contrast, a bipolar sensor will detect noninflected shapes easily, as they have a net positive or negative curvature. Multiple sensors with different characteristics may be added to a door panel or the side, front or any other surface of a vehicle to classify impacts by shape and to deploy air bags, air curtains, or other safety devices, depending on the shape class and the magnitude of the shapes over time. The outputs of the sensors may be combined arithmetically in an electronic processor by conventional analog or digital means. Combinations include arithmetic addition or subtraction, or logical AND and OR operations, based on each sensor triggering a binary logic state indicating the class of impact shape detected, and these logic states then being resolved by AND and OR combinatorial logic. It is also possible to combine responses within a single fiber, by providing multiple runs of the fiber across the region to be sensed, each coupled to the next through a turnaround loop. The combination will be a product of the individual sensor characteristics, which may be varied by type of treatment and by not inverting or inverting the treated portions with respect to convex or concave shapes. A sensor in which there is coupling between the two fibers due to a lenticular structure has throughput characteristics that are related to the attenuation effects exhibited by a single fiber, but modified by coupling effects that tend to counteract the attenuations of a single fiber. This suggests combining single fiber sensors with lenticularly coupled fiber sensors to better classify shapes. Such a combination will be described below, but first we will describe a lenticularly coupled sensor. For such a sensor to have a nonzero output, the curves must be of sufficient curvature to cause coupling from one fiber to the other, due to microbending or purposely applied enhanced coupling zones. For each curved region, there will be light coupled within the curved region. However, a curved region also attenuates light passing through either fiber toward other locations along the sensor structure, both in the emitting and receiving fiber. This causes the amount of light reaching the detector from multiple curved zones to be equal to or less than the amount from a single curved zone, for curvatures that each attenuate the light passing by them by half or more. For smaller attenuations, the throughput may increase and then fall off with increasing numbers of curves, or even continue increasing as more and more curves are added. The attenuation of signals from multiple curves is explained in the following way: Each curved zone attenuates light passing through it, from any source, due to microbending or purposely formed enhanced coupling zones or regions. Light coupled across at any curved zone will encounter transmission fiber losses from curves between the light source and the coupling zone or region, and receiving fiber losses from curves between the coupling zone or region and the detector. The number of curves imposing losses will be the same for any coupling zone, since zones nearer the detector will have fewer receiver fiber losses but more transmission fiber losses, and zones nearer the source will have fewer transmission fiber losses but more receiver fiber losses. For instance, a fiber structure with 6 equally curved zones along its length, wherein each curve imposes a local drop in throughput from 1.0 to 0.5, will have an overall throughput of 0.5 x 0.5 x 0.5 x 0.5 x 0.5 x 0.5=.016 for each zone of coupling. We apply only one loss figure at the region of coupling because coupling is distributed across the length of the curvature. If we consider that each curve would couple a unit amount of light if no attenuations occurred, then the total coupled throughput will be the sum of the attenuated unit amounts. Each attenuated coupled amount is 1.0 x 0.016 = 0.016, so the sum, or total throughput is .016 x 6 = 0.096. In contrast, an individual curve would have a throughput of 0.5 x 1.0=0.5, or more than 5 times more than the combined signal from the 6 curves. In this example, three curves would produce a throughput signal of 0.125 x 3 = 0.38 compared to the signal of 0.096 for six curves. The "6 curve" vs "3 curve" example is relevant to comparing the effects of a single dent to those of double dents, where each dent includes a positive and two negative curves of equal magnitude, and the coupling is monopolar (equal for any polarity of curvature). The double dents produce a signal almost 4 times smaller than a single dent of the same magnitude. If curves of different magnitudes are applied at different locations along a coupled fiber structure, then the net effect is of course complicated by the different amounts of coupled light, and the differing attenuations, at each curve. However, increasing curvature is associated with increasing coupling, so increased coupling is generally accompanied by increased attenuation, so the net throughput from multiple curves changes only slightly with changes in curvature of the individual curves. This is to be contrasted with the very robust increase in throughput for a single curve with increasing curvature. Even when the curvatures are varied along the coupled fibers, the attenuations are the same for light coupled at any of the curves, because both transmitter and receiver fibers have the same curves. The net throughput, Ec, for a coupled fiber sensor with n individual curves, each with unattenuated coupling Ki for light between the fibers, and attenuation Ai for light traveling down a fiber, is given by: (eq. 2) Ec = (IlAiX∑Ki), where the product J] and sum ∑ are taken over all i from initial to nth. Figure 20 is a graph of Ec vs. n, for various Ai from 0.1 to 0.9. The graph was created from a mathematical model in which each coupled throughput is assigned a normalized value of 1.0 before attenuations are applied. It can be seen that for increasing n, the net throughput either decreases, rises and then decreases, or continues to increase, as Ai is varied. For most fibers, the higher Ai values apply unless the curvatures are at the low end of values that produce measurable coupling. Note that in an actual sensor the unattenuated coupled throughputs would not have values of 1.0. Instead, they would be small for low curvatures and large for high curvatures, so that the absolute magnitudes of the family of plots in the graph would be different from that shown, usually opposite to that shown. However, the graph is only meant to indicate the variations for each single plot of the family, as the number of imposed curves is varied (by "plot" within a family, we mean what is usually called a "curve" within a family of curves, but have avoided the conventional term to avoid confusion with the spatial curves associated with the shape of fibers). The net throughput can be used as a measure of the shape of indentations in the side of a vehicle, such as to emphasize safety system deployment for sharp single dents vs. sharp double dents. By varying the type and placement of enhanced coupling zones and Ai, it is possible to create coupled fiber sensors that respond differently to different shapes. For instance a sensor with large fibers or with added enhanced coupling zones will respond to broader shapes than a sensor with very small fibers and/or no purposely added enhanced coupling zones. As another example, a sensor with low attenuation per bend might have an output that increases according to the number of dents, while another with high attenuation might have an output that decreases with the number of dents. As a further example, a coupled fiber sensor with added enhanced coupling zones could respond to a broad monotonic curvature, while an untreated sensor would not respond at all to a broad monotonic curvature. Multiple sensors with different characteristics may be added to a door panel or the side of a vehicle to classify impacts by shape and to deploy safety systems depending on the shape class and the magnitude of the shapes over time. The single fiber sensors of Figure 22 may be combined with lenticularly coupled fiber sensors of Figure 23 by extending the transmission fiber 12 of a lenticularly coupled sensor with a coupling region 20 formed of lenticular material 22 and fitting it with a second detector 18b as in Figure 24. The second detector 18b will respond to the net throughput of the transmission fiber 12 alone, the first detector 18a responding only to light coupled from fiber 12 to fiber 14. The outputs of the two sensors may be combined arithmetically or logically as described, so that both coupled and uncoupled responses may be obtained from the same structure for use in a shape classification function. The single fiber sensors of Figure 22 or Figure 23 are able to broaden the classification abilities achievable with a double fiber coupled sensor, since they have a different throughput equation when in use. In the latter embodiment, it is the same equation whether or not the "single fiber sensor" is a stand-alone device or is a portion of a double fiber sensor. While a double fiber coupled sensor has a throughput equation including product and sum terms (see eq. 2 above), the equation for a single fiber sensor has only the product term. Shapes including multiple curves, particularly multiple inflected curves, will result in different outputs from the single and double fiber sensors, beyond the obvious distinction that single fibers always have a throughput even when straight, which is not always true of double coupled fibers. An important property of a single fiber sensor with a nonlinear response to curvature magnitude is that its output can be made to decrease as more peaks or inflections are imposed, whereas a double fiber sensor can respond to the addition of peaks with little change in output. This means that it is possible to use the single and double fiber sensors together to resolve the number of peaks, and also to gain information about the magnitude of the applied curvatures. For example, in the case of a single fiber sensor that saturates at a certain positive curvature, its throughput remains constant for curvatures above a certain positive value. For a single dent (an inflected curve, or "peak") containing a curvature beyond the saturation value, its throughput will decrease. As more dents are applied, its net throughput will continue to decrease. In contrast, the throughput of a double fiber coupled sensor can be made to remain approximately the same as more dents are imposed, due to the summing term of equation 2. By comparing the outputs of the single and double fiber sensors, one may obtain information about the number of dents and their overall magnitude. The single fiber output will indicate number of dents, whereas the double fiber output will indicate magnitude of the curvature of the "sharpest" (highest spatial frequency) dent. The ability to classify shapes is a feature of sensors that are long compared to the highest spatial wavelengths present in the shape, particularly if it is possible to introduce nonlinearities or other local modifications to the magnitude response of the sensor. Nonlinearities permit obtaining useful outputs from sets of curvatures that would otherwise sum to zero. Other "tuning" factors are given in the example introduced in the following paragraph. The ability to tune the response of a long sensor to sense shape is an important aspect of the present invention, which distinguishes it from prior art. Shape classification may be performed with sensors of any technology that are able to combine curvature information along their lengths. Examples include capacitive bend sensors and resistive polymer bend sensors, as well as strain gauge bend sensors. An example of classification of shapes is given below, applicable to any sensor technology capable of measuring the integral or product of curvature along its length. Definitions used in the example are: Curvature: C= dθ/ds, where θ is the angular orientation of a space curve and s is the distance along that curve, regardless of its shape. The space curve is taken to be in cartesian space, with x and y coordinates. Curvature devolves to dθ/dx for shallow shapes, which is similar to the derivative of slope, or (dy/dx). This approximation is used in deriving beam equations (ref. Crandall and Dahl, An introduction to the mechanics of solids, McGraw-Hill, NY, p. 362, 1959), but does not hold well for sharp dents. Monotonic shape: a shape without inflections of curvature, i.e. the curvature is all of one sign (positive or negative). Inflected shape: a shape that contains both positive and negative curvatures. Note that this definition is for curvature (θ,s realm). In the x,y realm a shape can have monotonic (all positive or all negative) slope (such as a circular dent) but will still be inflected in the curvature realm. Dent: a synonym for inflected shape. Peak: a synonym for inflected shape. Integrated curvature: The integral of curvature along s. This is typically what a distributed fiber sensor reports, for all shapes applied along its length s. Local integration: It is important to point out that a fiber (or many other distributed sensors) perform local integration, reporting a single number at the output. This is what can make them "smart," if we are able to "tune" what is integrated. Local integration is what produces a zero result for a linear curvature sensor exposed to an inflected curve that starts and ends with zero slope. It is important to note that, for instance, the local integral of the absolute value of curvature will produce a large result, whereas the absolute value of the integral of curvature will produce a zero result for the inflected curve mentioned earlier in this paragraph. Sensors may integrate curvature along their lengths, or form a product of local or incremental curvatures. A product, if treated logarithmically, becomes an integral, as the logarithm of a product is the sum of the logarithms of the product factors. Also, a product of large (close to a normalized value of 1.0) throughputs that decrement by a small amount behaves approximately as 1 -(the sum of the decrements). Therefore, it is frequently permissible to view a product as an integral. Either can be used to perform classification according to the methods given in the description of the present invention. Tuning: Selecting the local sensors along a fiber (or other sensor) so that the integral is taken over functions including the following functions or their combinations (others are possible as well): a. absolute value of curvature. b. positive curvature only. c. negative curvature only. d. curvature that saturates at a chosen positive magnitude. e. curvature that saturates at a chosen negative magnitude. f. curvature selected through a spatial comb filter. g. responses that vary along s. In the present example, a table containing important classes for discrimination of accident events is provided. It shows discrimination is possible for most of these by using two sensors in combination. The sensors are of two types, called "1" and "2" with characteristics as described in the table. A third sensor described below is sufficient to discriminate a one remaining "problem" case. The third sensor is similar to sensors 1 and 2 but employs a specific saturation point for determining a particular class. The characteristics of sensors 1 , 2, and 3 are included in the description of various single and coupled fiber sensors given earlier in the description of the present invention. (Key to the table: si = sharp, inflected; si2 = two si dents; bi = broad inflected; bm = broad monotonic, 1xx = output of sensor 1 for xx dent; 2xx = output of sensor 2 for xx dent; xx = bi, bm, si, or bi). The logic indicated in the table will resolve all the shapes in a static or dynamic case except for the si2 case, which relies for detection on the magnitude of a positive output relative to another positive output. During the event, a small si2 output can look like an si1 output from a single dent that is very large, so additional classification means are required. The si2/si1 problem can be resolved by using a third sensor that saturates locally at a critical level of positive curvature and tends to ignore negative curvature. For this sensor, deepening si2 or si1 shapes will saturate at the same depth, causing the output to stop increasing at the same time. At (or after) that point in time, the magnitude of output from a NON-saturating sensor like no. 2 above can be used to infer whether it is an si2 or si1 event. The si2 event will always have a larger magnitude at sensor 2 when sensor 3 saturates, because it is like two si1 outputs added. Another means of resolving the si2/si1 problem is to use a coupled lenticular sensor. Such a sensor can be made to have a very small output for an si2 event, and a very large output for an si1 event, thereby resolving the problem with great simplicity. This completes our presentation of the present example. Figure 25 illustrates a coupled fiber sensor structure that, as in Figure 24, includes a detector 18a of light coupled from fiber 12 to fiber 14 and a detector 18b of light attenuated within the fiber 12 connected directly to the light source. The structure of Figure 25 further includes multiple bends or loops 60 so that the fibers may traverse the sensing region multiple times, multiple traverses being exposed to the same shapes, and so that the source and detectors may be co-located. With such a system, it is possible to use different enhanced coupling treatments on each traverse, so that the net signals are influenced by a combination of treatments. This amounts to a form of optical computer, wherein the optical signals are combined to infer shape information. The coupling region 20 is shown schematically as an oval shape following the overlapping fibers, representing a lenticular material 22. Alternatively, the coupling structure 20 may be discontinued at the bends or loops 60 to reduce coupling due to the bends or loops 60. Figure 21 shows a sinuated lenticularly coupled fiber sensor designed to provide a signal that decreases as it becomes covered by liquid. It may also be used to indicate the extent of contact with a solid surface or surfaces. The throughput of the sensor of Figure 21 may be calculated according to Equation 2. If the sinuations are equal and of moderate curvature, then the sensor in air will tend to have a net output that varies little with the number of sinuations, as indicated in the curve for Ai= 0.7 in Figure 20. As each sinuation becomes covered by liquid or contacts a solid, its coupling is decreased to near zero, so the sum term of Equation 2 is decremented by a single Ki as each sinuation is contacted. This results in a linear decrease in Ec as liquid or solid contact increases in extent, falling to near-zero throughput for total contact with all the sinuations. This is to be contrasted with a single fiber version of the sensor, with source and detector on the same single fiber. The throughput of such a sensor is determined by the internal reflection conditions at each curve. From experiments with individual curves, we know that the maximum attenuation that may be achieved at a single curve that has a covering of clear material to protect it is 33%. Thus, a single fiber sensor with successively immersed curves would be expected to have a throughput that varies in steps, the net throughput having values like 1.0, .67, 0.45, 0.30, 0.20, 0.14, etc. if the throughput for no contact is normalized to 1.0. This would be a useful sensor, except that it is very difficult in practice to achieve a 33% attenuation consistently. The attenuation value is highly dependent on the integrity of contact with the covering layer and the thickness and microscopic shape of the layer. This makes it difficult to form lookup tables in software to deal not only with the power law of the stepped attenuation function, but also with variability in each attenuation, which typically leads to attenuation values for single loops that vary from 10% to 33%. In contrast, the lenticularly coupled structure has a throughput that changes in equal steps down to near zero throughput, with each step dropping by 1/n where n is the number of sinuations. This is because frustration is virtually complete at each curve and the throughput is responding to the summation term of Equation 2. This evenly stepped behavior is little affected by small changes in the thickness or shape of the lenticular structure, or by contamination on its surface. Also, the small remaining throughput after total immersion can be measured to classify the medium contacting the sensor, according to its index of refraction. Typically, water with an index of 1.33 will produce approximately twice the residual throughput as hydrocarbons, with indices typically in the 1.4 to 1.5 range. The lenticularly coupled sensor structure is also useful for forming arrays where each member of the array is a lenticularly coupled sensor with either a single curve to detect contact at a point, or multiple curves to detect progress of a contact front along the curves of the member until a near-zero throughput is achieved and the next member begins responding to contact. It may be modified, for curves too gradual to have significant coupling due to microbending, by emphasizing loss and collection by purposely forming "loss" zones at the curved portions. An array of single point contact sensors formed from lenticularly coupled sensors each with a single curve and a single light detector, will produce very large changes at each detector, typically 90%, as the member associated with the detector comes into full contact with liquid or solid. If n sinuations replace the single sinuation of a point sensor, each detector will see changes that are approximately 1/n for contact with each sinuation. Thus it is possible to form arrays with members that exhibit either binary or quasi-continuous changes in throughput, each member having near-zero throughput for total immersion, with a small residual value indicating the type of medium present according to its index of refraction. Figures 26, 27 and 28 show two lenticularly coupled fibers 60, 62 from three different views. The curves in the fibers are of short radius, as the fibers are mounted in the end of tubing 72. The curves, or loops, 64 and 66, are adjacent and covered with a thin layer of optically transparent material 70, i.e., a clear epoxy. Both fibers are shown cut off short on one side of the loop, although that end may also be left uncut without consequence. The other, longer side is directed toward a light source or detector. As illustrated in Figure 26, a ray that is not within the plane of its loops is shown propagating upward in a first loop, where it exits the first loop near the apex. Although not explicitly shown in Figure 26, the ray exits at an angle directed toward the second loop or bend. As shown in Figure 26, the result of this transfer is shown by the downwardly directed arrows in the second fiber. Figures 27 and 28 indicate the out-of-plane egress of such rays near the apex of the first loop or bend of Figure 26, and their reentry into the second loop or bend, which involves an intermediate internal reflection from the optically transparent covering. Vertical arrows near the bottom of Figures 27 and 28 indicate the general overall direction of light within each loop, not specific mode angles. Not all of the light exits the loop or bend, but portions traveling around and past the loop or bend are, for simplicity, not shown in the figures. In a preferred embodiment for forming individual point sensors for a liquid sensing array, loop or bend radii approximately the diameter of the fiber are obtained by wrapping 0.25 mm diameter fibers tightly around the edge of 0.25 or 0.125 mm metal substrate. Other materials for use as substrates include other rigid elements such as polyester or glass suitable for use in the medium to be tested. For other sensors, such as array elements with multiple sinuations, loops or bends with larger diameters may be desirable, for instance to achieve an attenuation to produce a desired result from Equation 2. For other sensors such as a side impact shape sensor, the fibers may be straight initially. Figure 29 illustrates two elements of an array of paired loops or bends 78, built on the edge of a band of spring steel 80. In a typical array, the spring steel is 0.125 mm thick and 12.5 mm wide, and the fibers are 0.25 mm in diameter. As shown, the leftmost loop or bend of each pair carries light along the back side of the steel until it crosses over to the second loop or bend at the edge of the substrate. The light then travels along the second fiber along the front of the steel, toward a photodetector. The first loop or bend passes over the part of the second loop or bend at the back of the steel. During construction, the loops or bends are pulled tight so that the fibers touch the metal virtually everywhere along their lengths and are snug against each other and against the steel. If the steel band is narrow as shown, the natural curves of the fibers prevent orienting the long axes of the loops or bends perpendicular to the long axis of the steel, but this does not affect performance. The important factor is to achieve snug contact between fibers and to the metal. This occurs naturally, aided by the crossover of fibers and the tendency of the leads to both be placed in compression when the loops or bends are pulled tight. The loops or bends on the steel are covered in clear epoxy or a similar clear film 81 , and in fact the entire assembly is normally covered in epoxy. Only the loop or bend apexes need remain optically clear. The rest of the assembly can be covered with opaque materials. Figure 30 illustrates, in a simplified form, an array of four paired loops, as in Figure 29, attached to an interface box 82. While they are curing, but still flowable, epoxy or similar clear liquids naturally form the correct shape for transfer of light from one loop to the other. The requisite shape is lenticular, in that it follows the curve of the loops in one dimension, and is nearly flat or an outwardly convex dome shape between the loops. This shape is ideal for the three dimensional path taken by light transferring from one loop to the other. Light exits the first loop along its length, and is reflected by a curved length of the lenticular surface, with geometry well matched to the curved length of the second loop. Thus, light that exits the first loop at multiple points is very likely to enter the second loop in a geometrically symmetrical fashion. This result is evident in the high throughput of these sensors when exposed to air. Natural liquid forces such as capillary action cause uncured epoxy to flow in between the loops and to form a thin covering near the apexes. If optical throughput is observed during curing of the epoxy, it will be seen to improve during the initial part of the cure, when the epoxy is still capable of flowing. This is in contrast to coating two adjacent fibers cut square in the same plane. In that case, there is no transfer of light from one to the other, as the geometry deteriorates as the epoxy gets thinner on the cut faces of the fibers. For the cut fibers, there is simply not enough material on top of the cut faces for reflections to occur from one fiber to the other. The only cure would be to add a separately formed lens or reflective structure. The clear covering material is curved in one dimension, following the curved contour of the loops. This is a desirable shape, because it creates multiple reflection paths for the light emitted from the first fiber along a length of the loop. The curved shape is optimal for transferring light into the second fiber, which bears a symmetrical shape relationship to the first fiber. Single loop pairs as shown in Figures 26, 27 and 28 may be formed by bending the fibers into tight loops and pushing them back into surrounding tubing. The end can then be dipped in epoxy. At the non looped ends of the fibers, an LED or other light source is attached to one fiber for illumination, and the other fiber is attached to a photodiode and amplifier or other similar photodetection system. The cut end of each fiber near the sensing loops may be of any length, and can be extended to provide other signaling functions or to create other loop structures along the same fiber. Normally, however, it is cut 5 to 10 mm away from the loop. If desired, it may be covered with opaque material to prevent ingress or egress of light. An array according to the present invention may be used in conjunction with other devices. The optical sensor may be instrumented by attaching at least one fiber (a "first" fiber) from each pair to a light source, and the other fiber (the "second" fiber) to an individual photodetector. An array may also be multiplexed. For example, according to the above, an array may be used in a multiplexer whereby multiple first fibers are attached to each of several light emitting diodes (LEDs), and multiple second fibers are attached to each of multiple photodetectors. The fibers are arranged so that, for instance, four fibers from the first four looped or bent pairs of the array are illuminated by a first LED and the second looped or bent pair mates are read out by 4 photodetectors. The same 4 photodetectors are used to read out other pairs when they become illuminated by turning off the first LED and turning on another. This system may be extended to multiplex any number of loops. A typical multiplexer is arranged to have 6 LEDs and 8 photodiodes, with 8 fibers at each LED and 6 fibers at each photodiode, for a 6 X 8 = 48 element array. Alternatively, all loop or bend pairs may be illuminated by a common source, and read out by a television camera such as a charge-coupled- device (CCD) camera or a line scanner. An advantage of an array of discrete point sensors is the absolute accuracy with which the location of each loop is known along the substrate. When liquid first contacts a sensor pair, its location can be known with great accuracy. However, the position of liquid between point sensing pairs in an array is not known. This may be resolved by using another, continuous sensing means in conjunction with the array. The result can be a very accurate sensor combination. For example, a tank instrumented with a conventional pressure sensor has an approximate range of 1 % accuracy over the range of pressures due to changes in tank level. By combining the pressure sensor with an array of 16 optical point sensors according to the present invention, spaced equally over the height of the tank, the accuracy can be improved to as good as 1/16%, using a computer to re-calibrate the pressure sensor automatically every time the liquid level passes the accurately known position of one of the optical sensors. Similarly, 48 optical sensors could be used to obtain an overall accuracy of 1/48% = 0.02%. As illustrated in Figure 31 , an array, for example as illustrated in Figure 30, may also be used in conjunction with a standpipe inside the tank open at the bottom of the tank, and a means of varying the pressure locally within the standpipe to change the height of liquid within it. The control of local pressure requires only a small added pressure, as one need only vary the height by one inter-sensor distance. By reading the pressure over a span of one intersensor length of the array, combined with knowledge of the liquid location to the nearest intersensor interval, an instrumentation system can determine the actual liquid height before pressurization with excellent accuracy. For example, with the provision of a 48 element array and a 1 % pressure sensor, an accuracy of 1/48 percent is easily achieved over the total height of the tank. If desired, rather than use pressure to displace the liquid, one can also move the array up and down by known amounts to read the exact height of the liquid. A major advantage is that the array need not be moved by more than one intersensor length to determine the liquid height within the entire height of the tank. For instance, if there are 48 elements to the array, and the tank is 48 feet tall, there is no need to move the array more than 1 foot to determine the liquid height to great accuracy. An array of lenticularly coupled fiber sensors, each of which has multiple sinuations may also be used to obtain highly accurate measurements of liquid height. Each member of the array can be made to have a throughput that decreases by 1/n each time liquid covers one of the n sinuations in each member so that the member has a throughput near zero when fully covered. An array of 48 members, each with 10 sinuations, can have an absolute accuracy of 0.2 percent. In an alternative embodiment, the sensor may be used as a humidity sensor. In use one may detect the humidity in one's breath by breathing on the loops. As such, the device may be used as a small, rapid all optical humidity sensor substitute for a chilled mirror humidity sensor. Traditionally, one would chill the mirror to detect dew- point. By chilling the loops one would be able to detect dew-point. In a further alternative embodiment, a lenticularly coupled sensor with pre-formed curves that couple light between the fibers, may be used as a pressure sensor. According to the present alternative embodiment, the optical sensor includes a pair of fiber optic fibers, having a film, i.e., plastic or the like, placed against the loop or lens and pressure is then exerted on the film. Preferably the plastic film may be clear, colored or dark, and may even be opaque. Since the film is to some extent deformable, it will act as a frustrator (having an index higher than air, or in the case of dark tapes, simply an absorber) whose contact area varies with pressure. Performance is not affected by thickness of the contacting film. For example, films like 10 mil polyethylene, 4 mil mylar, 1 or 2 mil Scotch tape, black or colored vinyl tape and the like all produce similar results. This present alternative embodiment is a true index-based frustrator, not affected by light or dark colors on the other side of the film from the loops. A linear array of pressure sensors built according to this alternative embodiment, with a continuous sheath of flexible plastic between it and surrounding liquid, could be used to sense progress of the liquid along its length, according to the array members contacted by the plastic as the liquid advances, pushing the plastic against the members. In a further alternative embodiment, a lenticularly coupled sensor without pre-formed curves may be placed between two flexible indenting plates, such as waffle- patterned rubber sheets, plastic or metal screening, plates with holes or ridges, or the like. Pressure applied to the sheets will cause bending of the fibers and thus coupling of light between the fibers. The throughput of the sensor will be a measure of the applied pressure or force, and can be used to classify impressed pressure pattem shapes according to the curvatures imposed and the characteristic response designed into the sensor by various methods of creating enhanced coupling zones. In a further alternative embodiment shown in Figure 32, a pressure sensor array may be formed from multiple parallel fibers (fiber optic ribbon cable), by forming lenticular coupling regions 90 between adjacent fibers. If one coupling region per pair of fibers is formed, at a known position along the fibers, then the array may be used to sense magnitude and location of imposed pressure fields. Each coupling region may be formed by applying a clear flexible material so that it forms into a lenticular shape during curing, as explained previously. Coupling at lower curvatures may be enhanced by creating loss and collection zones under the lenticular structure. If the array is sandwiched between flexible indenting plates, such as waffle-patterned rubber sheets or screens, applied pressure will cause the fibers to bend and to couple light wherever a bend falls on a coupling region. Light sources 91 and detectors 92 may be placed at opposite ends of the ribbon, or reflectors may be applied to one end of the fiber ribbon, and all sources and receivers may be located at the other end. If reflectors are applied at one end of the cable to both receiving and transmitting fibers, then each coupling zone will couple direct and reflected light, resulting in a larger throughput. In a further alternative embodiment, a device including the paired optical fibers and lens would be quite sensitive to chemically activated gels or the like. If desired, a sensor could be used to allow for the detection of chemicals, for use as a chemical or biological activity detector or the like. Additionally, the device in accordance with the present invention could include a formed lens constructed from a material including dissolvable substances, such as a meltable wax, hot glue or the like. Such a sensor would be adapted to detect high temperatures or have the lenses dissolve in the presence of solvents. As discussed earlier, coupling across a lenticular zone may be enhanced by treating the fibers to lose and collect light, by methods such as abrasion or notching: "enhancement by treatment". Another enhancement means is to cover the lenticular zone with a reflective material such as vacuum deposited metal, adhered metal foil, reflective paints, epoxies, liquids, glasses, or thin films. Enhancement by means of a reflective layer will be referred to as "coupler mirroring". Enhancement by coupler mirroring alone can increase the throughput and reduce the effects of surrounding media. It will also tend to reduce light loss from the coupling zone over a wider range of curvatures, because internal reflections will tend to be independent of the angle of incidence of internal light with the outer surface. Enhancement by treatment can be used to reduce the curvatures at which coupling will occur. Sufficient treatment can produce coupling at zero curvature. However, a preferred method is to treat less and to also employ coupler mirroring, with both lens and mirrored surface surrounding both sides of the fibers. This has the effect of reducing the Ai terms of equation 2, so that coupling terms Ki predominate. The throughput is raised for straight fibers so that a bipolar sensor is easily produced; one that has decreasing throughput for bends of one polarity and increasing throughput for the other polarity. It is possible to make sensors that have a linear relationship between curvature and transversely coupled throughput. Single-fiber bend sensors have a drop in throughput when the treated zone is convex outward ('negative curvature polarity'). Transversely coupled bend sensors that include coupler mirroring and loss treatment have an increase in throughput for negative curvature polarity. Consideration is now given to the case where a lenticularly coupled pair of fibers has source and detector at one end of the pair and mirrored ends at the other end of the pair. Mirrored ends may be formed by conventional means such as vacuum deposition of metals, adhesion of metal or other reflective material, adhesion of microprisms, or prismatic cutting of the ends. Such a structure is shown in the perspective view of Figure 33, with a single, discrete lenticularly coupled zone. The lenticularly coupled zone may take on all the forms already discussed, including long, distributed; short, discrete; pre-bent; enhanced by 'loss' zones; not enhanced; lenticular on one side; lenticular on both sides; mirrored; or not mirrored. In all cases, light will couple transversely across the lenticular zone, according to the conditions of bend, loss treatment, and surrounding media. The structure of Figure 33 is the same as that of Figure 6 except for mirrored ends 111 and 113. The mirrored ends enable some new features. Light may now propagate across the coupling zone in both directions and be detected by the same detector. There is a 'direct' path, indicated by the figure numbers 101 , 102, 103, 104 and 105; and a 'reflected' path indicated by the figure numbers 101 , 106, 107, 108, and I09. Either end mirror may be removed and a detection path will remain, but when both mirrors are used there is more light. In Figure 33 the fibers are shown splayed apart to emphasize that the mirrors are separate so that the only coupling is across the lenticular coupling zone. In practice, the mirrored end portions of the fibers may be adjacent and touching, or touching but with the mirrors displaced axially. In a preferred embodiment, the structure of Figure 33 is a discrete curvature sensor, with adjacent mirrored ends, 0.5 mm diameter plastic optical fibers each treated to lose light in narrow adjacent strips 12 mm long, covered with a lenticular structure 110 of clear flexible epoxy surmounted with reflective foil. The source fiber 14 is powered by an LED with its optical output maintained constant in a control circuit; the detector fiber 15 is connected to a photodiode and transimpedence amplifier with an output voltage proportional to intensity of throughput light. A surface-treated area is indicated at 115. The following have been measured for such a structure: Throughput approximately doubles if both fibers are mirrored at the ends compared to only either one of the fibers. Without the mirroring on the lenticular coupling structure, throughput increases for negative bends (treated side convex outward), and decreases, but slightly, for positive bends. With the coupler mirroring, the throughput more than doubles and the response curve is truly bipolar and approximately linear. Modulation is approximately +/- 20% of throughput intensity for curvatures of +1-6 cm radius, with maximum throughput for negative bends. The same structure of Figure 33, without the coupler mirroring, becomes a pressure sensor if placed between two pieces of plastic screen with a mesh size of approximately 10 squares per cm. The plastic mesh is used to produce microbending and hence coupling between the fibers due to light lost into the lenticular structure. Pressure sensing of this sort may also be effected with the lenticular coupler but without the loss treatment. Typical output is a 10% increase in throughput for a pressure of 1 pound per square inch. The output may be increased by using metal bands such as %" x 0.005" spring steel on the sides of the screens facing away from the fibers. The same structure of Figure 33 may be extended to perform the same long-fiber shape sensing and liquid detection tasks described elsewhere in this disclosure for sensors not having reflectors on the fiber ends. In a further variation on the structure of Figure 33, a third fiber is added on the other side of the source fiber, adjacent to it so that all fibers lie in a plane. The third fiber is used as a second detector fiber, fitted with another optical intensity detector. Transverse coupling may be effected into either detector fiber at the same axial location or at separate axial locations. If coupler mirroring and loss treatment are applied, the attenuation term(s) Ai of eq. 2 will vary insignificantly with bending, so that each detector fiber may be used to measure either a different aspect of bending at the same location, or another bend at a different axial location. Examples of 'other aspect of bending' include bending sensed with a different linearity or polarity response, so that three fibers can be used to discriminate classes of shapes. In another embodiment, the fibers are arranged so their centers fall on corners of a triangle in cross section, rather than a line. A first set of loss treatment strips is applied so that light is coupled transversely from the source fiber to the first detector fiber along a side of the triangle. A second treatment is applied so that coupling occurs between the source fiber and the second detector fiber along another side of the triangle. A lenticular layer surrounds the entire structure or at least the coupling zones. Such a structure can sense bending along different axes, and be calibrated to become an 'X-Y' bend sensor, used to resolve a plane of maximum bending applied to the structure by a lateral force. To permit bending of the triangular structure, it may be constructed with somewhat extensible materials and/or twisted to form a spiral triangular structure. Larger arrays may be formed with multiples of the planar or triangular triads above. A larger planar array appears in Figure 32 in non-mirrored form, but the mirrored form is of course possible. Figure 34 is a schematic diagram of a lenticularly coupled fiber optic sensor as in Figure 33, but with multiple discrete coupling zones 84, 86, 88, 90. Each coupling zone may be made with the various treatments, mirroring, extents, and other variations discussed elsewhere in this disclosure. In this Figure mirrors are shown at 94, 96. In order to resolve responses at the detector due to deformations or interactions at each coupling zone, each coupling zone is made wavelength- dependent and the source fiber is illuminated with light of more than one wavelength, such as with white light, light from multiple LEDs, or a 'chirped' laser. Zones are made wavelength dependent by conventional means used to produce wavelength-dependent transmission or reflection. Means include coloring the lenticular medium with dyes, diffractive inclusions, or absorbers. Means also include coloring the reflective layer to be wavelength dependent, or using a dichroic thin-film reflective layer. Wavelength-selective detectors may be used at the detector end of the detector fiber, so that each detector responds to each coupler and not to the others. Means include detectors fitted with dichroic or colored filters, automated monochromators, diffraction grating spectrometers, and other conventional techniques. Using the same terminology as that for eq. 2, one can express the throughput of the structure of Figure 34. The first coupler, 84, has a direct path with throughput Ecd=K1 xA2xA3xA4xA4xA3xA2xA1 , and a reflected path throughput Ecr=K1 xA1 xA2xA3xA4xA4xA3xA2 Ecd and Ecr are the same. In fact, each coupler has an equation of similar form, so that for each coupler in this example: Ec1 =2xK1A1 x A2 Λ 2 x A3 Λ 2 x A4 Λ 2, where Ai Λ 2 is Ai x Ai. Ec2=2xK2A2 x A1 Λ 2 x A3 Λ 2 x A4 Λ 2 Ec3=2xK3A3 x A1 Λ 2 x A2 Λ 2 x A4 Λ 2 Ec4=2xK4A4 x A1 Λ 2 x A2 Λ 2 x A3 Λ 2 We wish to calibrate this system so that by measuring the separate Eci for each coupler, we may calculate Ki for that coupler, where Ki is the coupling factor due to an external influence (shape, pressure, contact, etc.). This is possible because in each case where the product is over all As except Ai for that coupler. The Ai can be taken to be constants if a reflective layer is used over the lenticular layer, in which case Eci=KiGi, where Gi is a constant associated with coupler i. If the Ai vary with bending, solutions are possible using recursive methods based on knowledge of the variations in Ai with bending for each coupler. An example of a wavelength-specific coupled structure used to make a three- dimensional bend and twist sensing structure as described (Danisch, 9F028-7- 7153/01 -SW) in the prior art, but now with only two fibers used to form the complete array, is given in Figure 35. The five coupled zones 84, 86, 88, 90, 92 are arranged at approximately 45 degrees to the axis of the common substrate 97 so that each senses a component of bend and twist. Once the curvature at each coupler is known, bend, twist, and full three dimensional cartesian shape are given in the prior art referenced above. Strong advantages may be cited for sensor structures built with reflectors at the ends: Source and detector may be located at a single end of the structure. Because no turn-around loops are necessary, the sensors may be built in long lengths and then cut to shorter lengths. End reflectors may be applied by thin film deposition, adhesion, spraying, or other low cost automated techniques. The structure may be as narrow as the fibers involved, with no additional space required for a turn-around loop. Further advantages result from reflectors at the coupling zones. For bend sensors, these act as optical buffers from external influences such as liquids and ambient light. The throughput is doubled, including modulated throughput, and less treatment is required to produce a bipolar bend sensor. As described above, single fibers, among other uses, enable the classifications of deformations. Thus, using two individual fibers, each treated differently to the other, such that each fiber produces a signal variation which is a product of the form of deformation. Thus, for example, one fiber can be treated such that it is particularly sensitive to long, relatively shallow deformations, while the other can be treated such that it is particularly sensitive to sharp-edged deformations. If applied to an automobile door, for example, and with the output from the fibers fed to a comparator, classification of the shape of the deformation can be obtained. This can be used to decide whether the deformation relates to a collision which warrants safety system actuation. Such fibers can be positioned in seats to determine whether the seat is occupied. If unoccupied then actuation of an air bag or other safety system is unnecessary. A seat application can be used also to determine the weight of an occupant, either preventing, or modifying, actuation of an air bag if the seat is occupied by a child or other small person. Many other uses can be considered. Further, more complex classification can be obtained by using more than two fibers. For example, in a multiple fiber arrangement, while some of the fibers may have the same treatment, their orientation can be varied, to provide some directional information regarding the deformation - giving what could be termed a "3D" result. Depending upon the information desired concerning the form, or shape, or size of a deformation, or any combination thereof, so a plurality of fibers can each have different treatments, or there can be combinations of fibers having different treatments and fibers having the same treatments but differently orientated. A common input can be used, but a separate detector is used for each fiber, the outputs being combined in a comparator for providing classification of the deformation. The treatment of the fibers can vary, typical examples being abrasion, chemical treatment, heat forming and notching. The type or form of treatment will vary in accordance with the particular form of deformation to be sensed, for example, coarse or fine notching, or abrasion. One form of treatment will be for monitoring short sharp deformations and another form of treatment for longer, more gradual deformations. In alternative embodiments, the device in accordance with the present invention could include a single fiber shape sensor for air bag or other safety system deployment decisions, including whether or not to deploy, at what pressure to deploy, based on a class of shape of an object striking a portion such as the front, sides or rear of a vehicle. In a further alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for determining a seat occupant weight, position and shape for purposes of safety system deployment decisions, including detection of an occupied child safety seat. Decisions for any of the above embodiments could be based on suitable methods and or programs, for example, algorithms in an electronic control system of a vehicle. In an additional alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor installed in a window, door or tailgate gasket or positioned in another suitable location, in order to detect if a hand or other body part if present. If such a body part is detected, the closure of the door, window or the like member would be interrupted. In a further preferred alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for detecting contact and the shape of contact between a car bumper or other vehicle, i.e. cars, trucks, constructions vehicles, front end loaders, boats, boat bumpers, loading docks, marine docks and other suitable surfaces where such a sensor would desirably be placed for detecting contact and shape of contact. In another alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for use in an alarm system, for example as an intrusion alarm on a threshold, under a rug, or other like object, or in a window or door structure. In an alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for a safety mat, to actuate or de-actuate a machine when a person steps on or off the mat. In an alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for use as a pressure detector buried in pavement or on pavement, to detect and measure vehicle wheel presence, shape, speed and numbers. Alternatively, according to the above, the single shape sensor could be used to detect, in a tire, under- or over-inflation, shape of the area of contact of the tire with the road, or the shape of any portion of the tire. In a further alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for use in a bed or chair, for detection of occupant position, weight, shape and other data for purposes of position adjustment, patient monitoring or sleep research. In an alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for use to detect contact and the force of contact in a target, such as a gaming target, gaming tool or military target. This would allow for measurement or detection of contact and force of contact of a ball, projectile or other like device. In an alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor for use in safety research, such as in or on the deformable elements of a crash-test dummy, i.e., in or on the deformable abdomen, chest or head of a crash-test dummy, to measure shape and severity of an impact. In an alternative embodiment, the device in accordance with the present invention could include a single fiber shape sensor in an elevator to detect the presence of an obstruction between the door or closing strips of the elevator doors. In a further alternative embodiment, the device in accordance with the present invention could include at least one fiber in a shape sensor adapted to detect the shape of frontal impacts for purposes of safety system deployment. As those skilled in the art will realize, these preferred illustrated details can be subjected to substantial variations, without affecting the function of the illustrated embodiment. Although embodiments of the invention have been described above, it is not limited thereto and it will be apparent to those skilled in the art that numerous modifications form part of the present invention insofar as they do not depart from the spirit, nature and scope of the claimed and described invention.

Claims: I CLAIM: 1. An optical sensing device comprising: a first optical lightguide; a second optical lightguide with a portion of its length parallel to and in close proximity to said first lightguide to form a coupling region; said first and second lightguides being covered within the coupling region; and wherein, intensity of light coupled from said first lightguide to said second lightguide is modulated, in response to a change in curvature of the lightguides out of their plane within the coupling region. 2. A device as claimed in claim 1 , wherein said cover for said coupling region is formed by a layer of optically transmissive material having a convex, arcuate outer surface. 3. A device as claimed in claim 2, wherein said optically transmissive material is surmounted by a reflective layer. 4. The device of claim 3, wherein the reflective layer is metallic. 5. The device of claim 3, wherein the optically transmissive layer is transmissive for a specific wavelength or range of wavelengths, wherein the specificity enables multiple coupling regions to be formed along the same pair of fibers and accessed separately by data acquisition means using specific wavelengths of light. 6. The device of claim 3, wherein the reflective layer is reflective for a specific wavelength or range of wavelengths, wherein the specificity enables multiple coupling regions to be formed along the same pair of fibers and accessed separately by data acquisition means using specific wavelengths of light. 7. A device as claimed in claim 1 , wherein the first and second lightguides are modified for enhanced coupling, by abrasion, chemical treatment, heat forming, or notching, to lose and collect light in adjacent surface areas facing away from the plane of the lightguides in the coupling regions. 8. A device as claimed in claim 2, wherein a covering layer is formed on only one side of the plane of the lightguides, thereby enabling coupling only for curvatures of the lightguides which impose convex curvature on the lens layer. 9. A device as claimed in claim 1 , means for injecting light into said first lightguide, and means for detecting the intensity of light coupled into said second lightguide. 10. A device as claimed in claim 1 , means for injecting light into said first lightguide, means for detecting the intensity of light coupled into said second lightguide, and means for detecting the intensity of light carried through said first lightguide. 11. A device as claimed in claim 2, wherein the covering layer is formed on only the side of the plane of the lightguides containing the loss and collection areas, thereby enabling coupling only for curvatures of the lightguides which impose convex curvature on the lens layer. 12. A device as claimed in claim 1 , said transparent material comprising a synthetic resin. 13. A device as claimed in claim 1 , said transparent material comprising a heat dissolvable material. 14. A device as claimed in claim 1 , said transparent material comprising a chemically removable material. 15. A device as claimed in claim 1 , said first and second lightguides formed into curves out of the plane of the lightguides, within the coupling region. 16. A pressure or shape measuring and classifying sensor as claimed in claim 1 , said first and second lightguides mounted on a surface to be deformed by imposed pressures or shapes. 17. A pressure or shape measuring and classifying sensor as claimed in claim 16, wherein the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that is maximal for only a single inflected shape and is attenuated when more than a single inflected shape is imposed. 18. A pressure or shape measuring and classifying sensor as claimed in claim 16, wherein the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that is maximal for shapes with large curvatures and minimal for shapes with minimal curvature. 19. A pressure or shape measuring and classifying sensor as claimed in claim 16, wherein the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that decreases for noninflected shapes and increases for inflected shapes. 20. A pressure or shape measuring and classifying sensor as claimed in claim 16, wherein the lightguide diameter and coupling enhancement means are chosen to produce coupled light intensity that is minimal for inflected shapes and maximal for noninflected shapes. 21. A pressure or shape classifying sensor comprising the first or second lightguide of claim 1 or claims 17 through 20 wherein the intensity of light that has passed through said lightguide is measured to classify the shape imposed on said lightguide according to the number of inflected curves, polarity of curvature, and magnitude of curvature. 22. A pressure or shape measuring and classifying sensor comprising: a first plurality of sensors as claimed in claim 1 , exposed to a distribution of curvature within an extent; a second plurality of sensors as claimed in claim 19, exposed to a distribution of curvature within said extent; wherein the measurements of a pressure or shape distribution by said sensors are analyzed singly and in combination to classify said distribution of curvature within said extent according to absolute value, polarity, number of inflections, number of peaks, spatial frequency content, and location within said extent, and to measure the time progress of said classifications. 23. A pressure or shape measuring and classifying sensor as claimed in claim 22, for determining classes and growth of impacted shapes in vehicles for purposes of air bag deployment. 24. A pressure or shape measuring and classifying sensor as claimed in claim 22 for determining occupant position and weight in vehicles for purposes of air bag deployment. 25. A pressure or shape sensing array comprising: sensors with coupling regions as claimed in claim 1 distributed over an area within which pressure or shape is to be measured at locations; wherein said sensor coupling regions are located to respond uniquely to pressure or shape at said locations; wherein the overall pressure or shape is inferred from the individual sensor measurements. 26. A pressure or shape measuring and classifying sensor array as claimed in claim 25, wherein the sensors comprise electrical conductors instead of lightguides, said coupling regions comprise electric coupling regions wherein coupling is modulated by bending, and said bending is determined by measuring electric current or voltage resulting from said coupling. 27. A pressure or shape sensing array as claimed in claim 25, wherein said sensors are formed from adjacent fiber pairs of a fiber optic ribbon cable, wherein each coupling region occupies a known location along the axial extent of said cable. 28. A sensor as claimed in claim 1 , 25 or 27 located between first and second mechanical layers, said mechanical layers containing structures capable of bending said sensors when pressure is applied. 29. A liquid or solid contact measurement sensor comprising the array as claimed in claim 25, said coupling regions preformed into curves that couple light maximally when surrounded by a medium of low index of refraction and which couple light minimally when surrounded by a medium of high index of refraction. 30. A liquid or solid contact measurement sensor comprising a sensor as claimed in claim 1 , with coupling regions preformed into curves along its extent, each curve of which couples light maximally when surrounded by a medium of low index of refraction and which couples light minimally when surrounded by a medium of high index of refraction. 31. A liquid or solid contact measurement sensor comprising the array as claimed in claim 29 in which a flexible surrounding material containing air at atmospheric pressure within is deflected by pressure from a liquid or solid medium without, to touch said curved coupling regions and produce changes in the measured intensity of light indicative of contact. 32. A sensor as claimed in claim 29, 30 or 31 , including a planar support member having an edge, said coupling regions spaced apart along and extending over said edge. 33. A sensor as claimed in claim 32, said coupling regions extending over said edge. 34. A liquid or solid contact measurement device as claimed in claim 1 , said coupling region preformed into a curve with its apex exposed at the end of a tube covering the device. 35. A liquid contact measurement device as claimed in claim 29 or 34, the intensity of coupled light when the device is immersed in liquid indicating the index of refraction of the liquid. 36. A liquid or solid contact measurement sensor as claimed in claim 29, whereby said array is adapted to indicate the level and composition of layered liquids. 37. A liquid or solid contact measurement sensor as claimed in claim 29, comprising an array with spaced sensors, and motive means for changing the liquid or solid level with respect to the sensor array by a known displacement up to one intersensor spacing, said array measurement and said displacement being used to determine liquid or solid height or composition along a continuum. 38. A method of sensing a pressure or shape comprising the steps of: providing a first optical lightguide; providing a second optical lightguide with a portion of its length parallel to and in close proximity to said first lightguide within a coupling region; covering said first and second lightguides within the coupling region, as a unit, by a lens layer of optically transmissive material having a convex, arcuate outer surface; transmitting light from a light source through said first optical lightguide; measuring the intensity of light coupled to said second lightguide through the lens layer, by measuring its intensity at the end of said second lightguide toward which said coupled light is directed, as a means of measuring curvatures within the coupling region. 39. A method of sensing liquid or solid contact comprising the steps of: providing a first optical lightguide; providing a second optical lightguide with a portion of its length parallel to and in close proximity to said first lightguide within a coupling region; covering said first and second lightguides within said coupling region, as a unit, by a lens layer of optically transmissive material having a convex, arcuate outer surface; forming said coupling region into at least a single curve; transmitting light from a light source through said first optical lightguide; measuring the intensity of light coupled to said second lightguide through the lens layer, by measuring its intensity at the end of said second lightguide toward which said coupled light is directed, as a means of measuring the contact of liquid or solid and the index of refraction of said liquid or solid. 40. An optical sensing device comprising : an optical lightguide; an actuation operable device associated with said optical lightguide; said optical lightguide when deformed forming a coupling region adapted to transmit light along its length when the lightguide is curved out of its plane by said actuation device. 41. A device as claimed in claim 40 including means for injecting light into said lightguide, and means for detecting the intensity of light coupled into said lightguide. 42. A device as claimed in claim 40, wherein there is provided a cover for said coupling region formed by a lens layer of optically transmissive material having a convex, arcuate outer surface. 43. A device as claimed in claim 40, wherein said lightguide is formed into curves out of the plane of said lightguide, within the coupling region. 44. A device as claimed in claim 40, wherein said lightguide is mounted on a surface to be deformed by imposed pressures or shapes. 45. A device as claimed in claim 40, for determining classes and growth of impacted shapes in vehicles for purposes of actuating an air bag actuation device. 46. A device as claimed in claim 45, for determining occupant position and weight in vehicles for purposes of air bag deployment 47. A device as claimed in claim 40, for determining classes and growth of impressed shapes along gaskets seals, trim, and panels. 48. A device as claimed in claim 40, wherein said lightguide is mounted in a surface to be deformed by imposed pressures or shapes for purposes of determining classes and growth of impacted shapes. 49. A device as claimed in claim 1 , wherein said lightguides are mounted in a surface to be deformed by imposed pressures or shapes for purposes of determining classes and growth of impacted shapes 50. An optical sensing device comprising: at least two separate optical lightguides, each having an input and an output, the lightguides treated differently one to the other to produce a signal variation, and means for comparing the signals to provide the classification of a deformation. 51. A device as claimed in claim 50, comprising a pair of optical lightguides extending side by side. 52. A device as claimed in claim 50, comprising a plurality of optical lightguides, including at least two lightguides having different treatments, and at least two lightguides having the same treatment but having different orientation. 53. A device as claimed in claim 50, one fiber sensitive to long shallow deformations and the other fiber sensitive to short sharp deformations. 54. A device as claimed in claim 1 , at least one of said optical lightguides having a mirrored end surface. 55. A device as claimed in claim 1 , said first lightguide having an input end, a light source connected to said inlet end and a mirror at its other end, said second lightguide having an output end, a detector means connected to the output end, a mirror at its other end, and at least one coupling region. 56. A pressure or shape measuring and classifying sensor as claimed in claim 1 or claim 50, for determining classes and growth of impacted shapes in vehicles for purposes of air bag deployment.

Inventors: DANISCH LEE A, DANISCH, LEE, A.
Applicants: DANISCH LEE A, DANISCH, LEE, A.
Application year: 2000
Main classification: G01D5
IPC codes: B60R21, G01D5, G01F23, G01G3, G01G19, G01L1, G01L11, G01N21