Compact optics for concentration, aggregation and illumination of light energy

Information

  • Patent Grant
  • 7925129
  • Patent Number
    7,925,129
  • Date Filed
    Friday, February 12, 2010
    14 years ago
  • Date Issued
    Tuesday, April 12, 2011
    13 years ago
Abstract
A solar concentrator having a concentrator element for collecting input light, a redirecting component with a plurality of incremental steps for receiving the light and also for redirecting the light, and a waveguide including a plurality of incremental portions enabling collection and concentration of the light onto a receiver. Other systems replace the receiver by a light source so system optics can provide illumination.
Description

This invention is directed to a solar concentrator for producing electrical, thermal and radiative energy. More particularly, the invention is directed to a solar concentrator using a combination of refractive and reflective and/or redirecting optics to concentrate and aggregate sunlight from a plurality of concentrator systems. Other applications include lighting and illumination using the compact optics.


BACKGROUND OF THE INVENTION

Solar collectors have long been developed for the collection and concentration of sunlight. Increasing the energy density of ambient sunlight enables more efficient conversion to useful forms of energy. Numerous geometries and systems have been developed, but the mediocre performance and high costs of such systems do not permit widespread use. In order to achieve adequate performance and manufacturability, improvements in solar energy collectors are needed.


SUMMARY OF THE INVENTION

A concentrator system includes a combination of optical elements comprising a concentrating element, such as a refractive and/or reflective component, a reflective and/or refractive element to redirect sunlight into a light waveguide which is constructed with a plurality of stepped reflective surfaces for efficient aggregation and concentration into a receiver unit (thermal and/or photovoltaic) and other conventional energy conversion systems. The control of the geometry of the reflective surfaces along with the aspect ratio of the light waveguide enables ready manipulation, collection and concentration of sunlight preferably onto a contiguous area for a variety of commercial applications, including solar cell devices, light pipe applications, heat exchangers, fuel production systems, spectrum splitters and other secondary manipulation of the light for various optical applications.


These and other objects, advantages and applications of the invention, together with the organization and manner of operation thereof, will become apparent from the following detailed description when taken in conjunction with the accompanying drawings.





BRIEF DESCRIPTION OF THE DRAWINGS


FIG. 1 illustrates a solar energy concentrator generally constructed in accordance with an embodiment of the invention;



FIG. 2 illustrates a cross-sectional view of one embodiment of a light waveguide shown schematically in FIG. 1;



FIG. 3 illustrates another cross-sectional view of a linear embodiment of a light waveguide shown schematically in FIG. 1;



FIG. 4 illustrates another cross-sectional view of a rotational embodiment of a light waveguide shown schematically in FIG. 1;



FIG. 5A shows a first edge shape of a reflecting element of a waveguide; FIG. 5B shows a second edge shape for a reflecting element of a waveguide; FIG. 5C shows a first separate element for redirecting light as part of a stepped waveguide; FIG. 5D shows a second separate element for redirecting light as part of a stepped waveguide; FIG. 5E shows a system with plural light pipes coupled to a stepped waveguide and FIG. 5F shows a waveguide with embedded redirecting components;



FIG. 6 shows a curved concentrating element and curved reflector coupled to a waveguide;



FIG. 7 shows a curved concentrating element and two planar reflectors coupled to a waveguide;



FIG. 8A shows a closed optical element coupled to a waveguide and FIG. 8B shows an enlarged view of a portion of FIG. 8A at the juncture of the optical element and waveguide;



FIG. 9A shows another closed optical element coupled to a waveguide and FIG. 9B shows an enlarged view of a portion of FIG. 9A at the juncture of the optical element and the waveguide;



FIG. 10A shows another closed optical element coupled to a waveguide and FIG. 10B shows an enlarged view of a portion of FIG. 10A at a juncture of the optical element and the waveguide;



FIG. 11A shows a further closed element coupled to a waveguide and FIG. 11B shows an enlarged view of portion of FIG. 11A at a juncture of the optical element and the waveguide; and



FIG. 12 shows ray tracing results for the optical systems of FIGS. 2 and 6-11.



FIG. 13 illustrates another representation of an embodiment of a solar energy concentrator or an illuminator;



FIG. 14 illustrates a refractive concentrator component for a conventional system;



FIG. 15 illustrates a reflective concentrator component for another conventional system;



FIG. 16 illustrates a Cassegrainian concentrator having a primary and secondary reflective optic;



FIG. 17 illustrates light transmission versus acceptance angle for a system like FIG. 13.



FIG. 18 illustrates an embodiment where the waveguide ends with a reflector component for redirecting light towards a base surface;



FIG. 19 illustrates a variation on FIG. 18 where the concentrator is mirrored about an axis of symmetry;



FIG. 20 illustrates a form of the embodiment of FIG. 13 with the waveguide and redirecting elements tilted relative to the concentrators;



FIG. 21 illustrates an embodiment with varying size of concentrator and/or redirecting element;



FIG. 22 illustrates an embodiment for light diffusion using a light source in place of a receiver;



FIG. 23 illustrates a different variation on the embodiment of FIG. 4 to achieve light concentration across two axes;



FIG. 24 illustrates yet another embodiment to achieve concentration across two axes;



FIG. 25 illustrates a different embodiment of a solar concentrator of the invention;



FIG. 26 illustrates yet another embodiment of a solar concentrator of the invention;



FIG. 27 illustrates a further embodiment of a solar concentrator of the invention.





DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

A solar energy concentrator system constructed in accordance with a preferred embodiment of the invention is indicated schematically at 10 in FIG. 1. The solar energy concentrator system 10, includes an optical concentrating element 12 which can be any conventional optical concentrator, such as an objective lens, a Fresnel lens, and/or a reflective surface element, such as a parabolic or compound shaped reflector. This optical concentrating element 12 acts on input light 14 to concentrate the light 14 to a small focal area 16. In the preferred embodiment, the small focal area 16 is disposed within reflective or redirecting component 18, or other conventional optical redirecting element which causes total internal reflection. The redirecting component 18 redirects the concentrated light 20 into a waveguide 22. The waveguide 22 is constructed to cause internal reflection of the light 20 which propagates along the waveguide 22 in accordance with Snell's law wherein total internal reflection occurs when the angle of the light 20 incident on surface 24 of the waveguide 22 is greater than the critical angle, Øc:

Øc=sin(ηwaveguidecladding)


Where Øc=critical angle for total internal reflection,


ηwaveguide=refractive index of waveguide material


ηcladding=refractive index of a cladding layer or the index at the ambient/waveguide interface.


A receiver 26 is disposed at the end of the waveguide 22 and receives the light 20 for processing into useful energy or other optical applications.



FIG. 13 illustrates a preferred form of the system 10 with details of this mechanism. A plurality N of concentrating elements 12 and redirecting elements 18 are shown. Each of the concentrating elements 12 takes the input light 14 with a half angle of θ1 from an area A, and concentrates the light 14 to a smaller area B with half angle θ2, such that Concentration Ratio=A/B. Each of the redirecting elements 18 receives the concentrated light from an associated one of the concentrating elements 12, rotates it by some angle φ, and inserts it into a section of the waveguide 22, preserving the level of concentration defined by area B and half angle θ2. The waveguide 22 is a plurality of sections having incremental steps of height B that are spaced from each other by length A. Each section of the waveguide 22 receives light from an associated one of the redirecting elements 18, such that the waveguide 22 as a whole aggregates light from the plurality of the concentrating elements 14 and the redirecting elements 18, and propagates the light 14 along its length for collection by a receiver 23. The waveguide 22 does not change the level of concentration delivered to it, and therefore the aspect ratio of the waveguide 22











=


height





of






waveguide
/
length






of





waveguide









=


N
×

B
/
N

×
A









=


B
/
A









=


1
/
Concentration






Ratio





in





each





element









Compactness has great practical benefits for solar concentrators (and other devices such as illuminators). Among other benefits: less material is used, large air gaps between optics and the receiver 23 that need difficult sealing are eliminated, devices are much less bulky for cheaper shipping and installation, traditional flat module manufacturing methods can be utilized as opposed to expensive and risky custom manufacturing methods.


The limit of compactness for the waveguide 22 is defined by the receiver 23. Thus, the waveguide 22 can only be as compact as the receiver 23 to which it delivers light. For most concentrators, the compactness of the concentrator 12 is significantly larger than the width of the receiver 23. However, since this device constructs the waveguide 22 from sections each having height defined by the area of concentrated light delivered to it, the aggregated waveguide 22 has a height equal to the width of the receiver 23. In other words, the waveguide 22 is at the limit, of compactness.


Therefore in view of the construction of the invention, the concentration of light achieved by the concentrator system 10 being a function of the aspect ratio A/B leads to a highly compact concentrator system 10. The device can aggregate light from a relatively wide area and concentrate it to a relatively small receiver that has a contiguous area while remaining highly compact. This simplifies production by reducing the volume of material required, allowing for multiple units to be made from a single mold and reducing assembly complexity.



FIG. 12 shows the results of ray tracings performed on the designs depicted in FIGS. 2 and 6-11. Each design demonstrates a particular performance in terms of its ability to concentrate light in the linear dimension, as shown by the ratio of A/B. The data is for light having an input cone half angle of +−1 degree, an output cone half angle of +−20 degrees, an initial refractive index of n=1, and a final refractive index of n=1.5. The theoretical maximum allowable concentration of light with those input parameters is 30× in the linear dimension, whereas FIG. 9 for example achieves a concentration factor of 25×. Since the concentration factor in the linear dimension is proportional to the aspect ratio A/B, the design shown in FIG. 9 can deliver a concentrator that is 250 millimeters long (A) while only 10 millimeters in thickness (B); or a concentrator that is 500 millimeters long (A) while only 20 millimeters in thickness (B). This represents a highly compact concentrator system 10 that can effectively aggregate concentrated light from a relatively wide area and deliver it to a single receiver.


The dimensions and number of the concentrating elements 12 and redirecting elements 18 can be varied for any entry aperture of the concentrator 12. For example, the system 10 shown in FIG. 13 can be achieved with twice as many elements (2×N) of half the size (A/2 and B/2). As the concentrating elements 12 and the redirecting elements 18 become smaller and more numerous; the aspect ratio of the entire concentrator 12 approaches the aspect ratio of the waveguide 22, given by 1/Concentration Ratio. In other words, for a Concentration Ratio of 10, the aspect ratio of the concentrator 12 can be 0.1.


Typical aspect ratios for concentrators 12 are on the order of 1. FIG. 14 shows a refractive concentrator 12, which may be, for example, an objective lens or a Fresnel lens. The focal length of an objective lens defines the height 25. The Concentration Ratio is given by A/B, whereas the aspect ratio is given by height/A, which is larger than the Concentration Ratio. FIG. 15 shows a similar situation for a reflective form of the concentrator 12.


Attempts have been made to reach the limit of compactness for a single concentrating element. FIG. 16 shows a Cassegrainian concentrator composed of a primary and secondary reflective optic. The aspect ratio given by Height/A is 0.25. Winston, in “Planar Concentrators Near the Etendue Limit”, 2005, describes the “fundamental compactness limit of a ¼ aspect ratio.” In the context of the invention, this compactness limit applies to an individual one of the concentrating elements 12. The use of the waveguide 22 that aggregates light from multiple ones of the concentrating elements 12 is what allows the compactness of the system 10 to go lower than ¼ and approach 1/Concentration Ratio.


The invention also has advantages in the transmission efficiency of light energy from input to delivery to the receiver 23. In FIG. 13, θ2 is controlled by the concentrating element 12. θ2 also becomes the angle made by the light hitting the surface of the waveguide 22, and 90-θ2 is the angle made with respect to the normal of the waveguide surface. As discussed above, θ2 can be set to achieve total internal reflection within the waveguide 22, reducing surface absorption losses to zero.


In addition, the concentrating element 12 and redirecting element 18 can be designed to manipulate the light 14 using total internal reflection, as shown in specific embodiments below. Also, the concentrating element 12 and redirecting element 18 and the waveguide 22 can be designed to provide a contiguous path within a solid dielectric medium for the light 14. In other words, light rays from the input region to the receiver 23 need never encounter either a reflective coating or a change in refractive index. Reflective coatings can cause absorption losses of ˜8%. A change in refractive index from an optical material of refractive index 1.5 (plastic or glass) to air can cause Fresnel reflection losses of ˜4%. Transmission efficiency with respect to these loss mechanisms can therefore approach 100%.


This is in contrast to conventional concentrator optics. Reflective optics will have 8% loss per reflection. Transmission efficiency will therefore be ˜92% for a single optic, and ˜85% when a secondary reflective optic is used. Refractive optics require at least one change in refractive index. Transmission efficiency will therefore be ˜96% for a single optic, and ˜92% when a secondary refractive optic is used.



FIG. 17 shows transmission as a function of input half angle θ1 through the embodiment of the invention shown in FIG. 13. The calculation is based on ray tracing software. The embodiment was designed to function within input angles of +−3 degrees. The efficiency takes into account losses from Fresnel reflections and hard reflections. As is shown, the efficiency of the device approaches 100% at θ1=0 degrees, stays near 100% within +−3 degrees, and then drops off sharply.


In another preferred form of the concentrator system 10 shown in FIG. 2, the incident light 14 is concentrated or focused in a first step using the element 12 described hereinbefore. The concentrated light 20 is further processed by associating sections of the concentrator system 10 with reflector/waveguide sections 28. Each of the reflector/waveguide sections 28 comprises a reflective section 32 which receives the concentrated light 20 and redirects light 30 within the associated waveguide section 28 with the light 30 undergoing total internal reflection (TIR) along the length of the entire waveguide 22. A plurality of the reflector/waveguide sections 28 comprise the waveguide 22 and forms a stepped form of waveguide construction.



FIG. 18 shows another embodiment of the system 10 where the waveguide 22 ends in a reflector 27 that redirects the light 14 towards the base surface of the waveguide 22, where the receiver 23 may be placed. It can be of manufacturing benefit to have the concentrator optics be laid down flat onto a plane of conventional receiver elements which embody the receiver 23.


With this construction, the concentrator 12 can be mirrored about an axis of symmetry as shown in FIG. 19, such that the two receivers 23 from either end form one contiguous area where one single receiver 23 may be placed. In this case, since the aperture area is doubled but the thickness of the concentrator 12 unchanged, the limit of compactness is given by 1/(2× Concentration Ratio).


The redirecting element 18 rotates the light paths by an angle φ. In FIG. 13, φ is shown to be 90 degrees. FIG. 20 depicts y<90 degrees. This can allow, as one benefit, the concentrating elements 12 to be located on the same plane, and the redirecting elements 18 on their own plane as well, which can aid manufacturability.


The concentrating element 12 and the redirecting element 18, and associated waveguides 22, may also vary in size and FIG. 21 shows an example of this. Here A1, A2, and A3 are different lengths, as are B1, B2 and B3. However, the Concentration Ratio stays the same in each section: A1/B1=A2/B2, and so on. The aspect ratio of the waveguide 22 is therefore still given by











=



(


B





1

+

B





2

+

B





3


)

/

(


A





1

+

A





2

+

A





3


)










=


1
/
Concentration






Ratio







In another embodiment shown in FIG. 22, the system 10 can also be utilized as a light diffuser by running light 31 through it in reverse. In FIG. 22, light input from a light source 33 that was originally the receiver 23, is channeled through the waveguide 22, redirected by the redirecting element 18 onto the concentrating element 12, which delivers the output light above the system 10. Applications include illumination, backlighting, and other light diffusing devices. It should be understood throughout that optics illustrated for concentration of light can also be used for illumination with the “receiver 23” being replaced by a light source.


The cross-section of the various reflector/waveguide sections 28 provides a basic building block for various configurations of the concentrator system 10. One exemplary commercial embodiment is shown in FIG. 3 with an aspect ratio N×B/N×A, A/B, an area concentration factor or energy density ΔØ which is proportional to A/B where N×A is the length of the waveguide 22 and N×B is the largest thickness (see FIGS. 2 and 3). In a most preferred embodiment, the thickness N×B is comprised of a plurality of incremental step heights, B, which provide a clear light pathway for TIR light from each of the reflector/waveguide sections 32.



FIG. 4 illustrates another example of the concentrator system 10 in the form of a rotationally (or axially) symmetric geometry having a concentrator system 10′ and the concentrating element 12 in association with the reflector/waveguide sections 28 of the waveguide 22. This rotationally symmetric form of the concentrator system 10′ (or the system 10), which can be any portion of a full circle, enables three dimensional radial convergence of the incident light 14 resulting in ΔØ the Concentration Ratio being proportional to (A/B)2 thereby substantially enhancing collection and concentrator efficiency. In a most preferable embodiment of FIG. 4 two axis solar tracking is used as opposed to the single axis tracking for the embodiment of FIG. 3.



FIG. 4 shows one way to achieve concentration across two axes, and FIG. 23 shows another way. Here, a linearly symmetric primary concentrator 12 delivers light concentrated along one axis to its receiver 23 at the side of a concentrator 12. There, a second linearly symmetric concentrator 37 is positioned in the perpendicular axis. This secondary concentrator 37 concentrates light along the second axis, bringing the light to the final receiver 23.



FIG. 24 shows a third way to achieve concentration across two axes. Here the concentrators 12 shown are of the mirror symmetry as described in FIG. 19. Again, a linearly symmetric primary concentrator 12 delivers light 14 concentrated along one axis to its receiver 23 at the base of the concentrator 12. There, a second linearly symmetric concentrator 37 is positioned in the perpendicular axis. This secondary concentrator 37 concentrates the light 14 along the second axis, bringing the light to the final receiver 23.


In addition to the linear and rotational embodiments of FIGS. 3 and 4, the concentrator system 10′ can be disposed both above and/or below the waveguide 22 relative to the direction of the incident light 14. In such embodiments, some of the light 14 will pass through the waveguide 22 and be redirected back to the waveguide 22 by the concentrator system 10′. These forms of systems enable light recycling and thus improve end efficiency and the use of the reflective systems for concentration, described herein, show an increased efficiency for concentration of light relative to conventional refractive system.


In other embodiments, the reflective elements 18 can be angularly adjusted with respect to the waveguide 22 in order to cause TIR. The reflective element 18 can be an integral part of the waveguide 22 with a variety of angular profiles (see FIGS. 5A and 5B). The element 18 also can be separate elements 38 and 39 (see FIGS. 5C and 5D). In addition, the reflective element 18 and the associated waveguide 22 can also take the form of complex light collector pipes 42 and light redirecting components 43 as shown in FIGS. 5E and 5F, respectively.


The above described forms of the concentrator system 10 and 10′ provide concentrated light 20 to a contiguous area as opposed to a nodal area, thereby allowing delivery of concentrated solar energy to a variety of downstream receivers 26, such as a solar cell, a light pipe for further processing, a heat exchanger, a secondary concentrator and a light spectrum splitter.


In yet another series of embodiments shown in FIGS. 6-11B, a variety of optical components can be used in combination to further and substantially enhance both the concentration and collection efficiency. FIG. 6 in a most preferred embodiment shows a curved concentrating element 50 directing light 52 onto a curved reflector 54 which passes the light 52 into the waveguide 22. FIG. 7 in another most preferred embodiment shows another curved concentrating element 56 which directs the light 52 off a reflector 58 having two planar surfaces 59 and 60 which redirect the light 52 by TIR into the waveguide 22. FIG. 8A shows a partially closed optical element 64 which redirects the light 52 at interface 66, reflects the light 52 off curved reflector 68 focusing the light 52 onto interface 70 between a bottom reflective surface 72 of the optical element 64. As best seen in the enlarged view of FIG. 8B, the waveguide 22 has a substantially complementary angular match to the reflective surface 72.


In FIG. 9A in another most preferred embodiment is a similar system as in FIG. 8A, but the optical element 65 is closed and coupled to an extension waveguide 74 (a form of light pipe) which collects the light 52 and transmits it into the waveguide 22 (as best seen in FIG. 9B).


In FIG. 10A an optical element 76 is closed with the input light 52 reflected by TIR from reflective surface 77 with a particular angular cross section best shown in FIG. 10B which enables collection of the light from TIR and coupling with the waveguide 22 from reflection off surfaces 80, 81 and 82.


In FIG. 11A an optical element 82 cooperates with another reflector 84 to direct the light 52 into the waveguide 22 from the two different optical sources 82 and 84, thereby further ensuring collection of all the light incident on surface 86 of the optical element 82. In this embodiment the optical elements 82 and 84 perform the role of both concentrating elements and reflecting elements.


In FIG. 25, a curved concentrating element 12 directs the light 14 onto (the redirecting component 18) which passes the light 14 into the waveguide 22. The concentrating element 12 and the redirecting component 18 are shown as two different features on the same physical part, while the waveguide 22 is shown as a second physical part coupled to the first. In FIG. 26, a curved concentrating element 12 directs the light 14 onto two reflectors (the redirecting component 18) acting in sequence which pass the light 14 into the waveguide 22. The concentrating element 12, the redirecting component 18, and waveguide 22 are all shown as separate physical parts coupled together. FIG. 27 directs the light 14 into the waveguide 22 similar to FIG. 26. However, the redirecting component 18 and the waveguide 22 are combined into one construction.


The foregoing description of embodiments of the present invention has been presented for purposes of illustration and description. It is not intended to be exhaustive or to limit the present invention to the precise form disclosed, and modifications and variations are possible in light of the above teachings or may be acquired from practice of the present invention. The embodiments were chosen and described in order to explain the principles of the present invention and its practical application to enable one skilled in the art to utilize the present invention in various embodiments, and with various modifications, as are suited to the particular use contemplated.

Claims
  • 1. An optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a concentrating element for collecting and repositioning light; andb) an associated redirecting element which is optically associated with and physically separate from the concentrating element for receiving light from the concentrating element, wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction, and the layer being contiguous between at least a portion of each of the associated redirecting elements;the optical concentrator further including a stepped waveguide for receiving the light from the at least one portion of the associated redirecting element which is constructed to reposition the light into the stepped waveguide for accumulation, the waveguide aggregating the light from the plurality of optical elements to provide optical concentration of the light for use thereof.
  • 2. The optical concentrator as defined in claim 1 wherein the plurality of optical elements and the stepped waveguide each form a contiguous layer and are disposed in a stack of physically separate components, thereby enabling direct assembly of separate parts comprising the optical concentrator.
  • 3. The optical concentrator as defined in claim 1 wherein the waveguide includes an upper and a lower element which are substantially parallel.
  • 4. The optical concentrator as defined in claim 1 wherein the optical elements are selected from the group consisting of a parabolic surface, an elliptical surface, a hyperbolic surface, an arc, a flat reflective surface, a tailored shape reflective surface, a total internal reflecting surface, a compound parabolic concentrator optic, a refractive component selected from the group of a spherical component, an aspherical component, a Fresnel lens, a cylindrical lens and a tailored shape.
  • 5. The optical concentrator as defined in claim 1 wherein the optical concentrator is linearly symmetric.
  • 6. The optical concentrator as defined in claim 1 wherein the optical concentrator is rotationally symmetric.
  • 7. The optical concentrator as defined in claim 1 wherein the optical concentrator further includes a receiver which collects the aggregated light for use thereof.
  • 8. The optical concentrator as defined in claim 1 wherein the concentrating element is comprised of a combination of (1) a surface between a high index material and a low index material enabling refraction of input light and (2) a parabolic reflective surface which repositions the input light with the combination outputting the input light without the input light being repositioned more than once by the parabolic reflective surface.
  • 9. The optical concentrator as defined in claim 1 wherein an end of the stepped waveguide comprises additional optical features that redirect the light from the waveguide towards a receiver.
  • 10. The optical concentrator as defined in claim 1 where the plurality of optical elements and the stepped waveguide are mirrored about a central axis to form at least two systems, such that a receiver in each of the at least two systems combine to form one contiguous receiver, and the optical concentrator comprises an increased width of at least about twice that of one system while retaining a same height.
  • 11. The optical concentrator as defined in claim 1 wherein the concentrating element and the redirecting element have a size selected from the group of about the same size and varying size.
  • 12. A optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including a concentrator element for collecting and repositioning input light;and the optical concentrator further including:a waveguide comprised of a plurality of portions with each of the portions associated with one of the concentrating elements, each of the waveguide portions further having a feature associated with receiving the output light from the concentrating element, the waveguide aggregating the light from the plurality of optical elements;wherein the plurality of optical elements and the waveguide each form contiguous horizontal layers disposed in a vertical stack.
  • 13. An optical system for processing light from a light source to provide illumination output, comprising: a stepped waveguide for collecting input light from a light source and delivering the input light to step features of the stepped waveguide;a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a redirecting element for receiving the input light from the stepped waveguide and repositioning the input light;b) an associated concentrating element which is associated with and separate from the redirecting element for receiving light from the redirecting element and diffusing the light for output therefrom to provide the illumination output, wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction and the layer being contiguous between at least a portion of each of the associated redirecting elements.
  • 14. An optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a refracting concentrator element for collecting and repositioning light; andb) an associated redirecting element which is associated with and separate from the concentrating element for receiving the light from the concentrating element wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction and the layer being contiguous between at least a portion of each of the optical elements;and the optical concentrator further including:a waveguide for receiving the light from the at least one portion of the associated redirecting element which is constructed to reposition the light into the waveguide for accumulation, the redirecting element being an integral part of the waveguide, the waveguide having top and bottom surfaces that are substantially parallel, the waveguide having a substantially uniform thickness along its length, and the optical elements constructed so as to insert the light into the waveguide such that light is propagated multi-directionally within the waveguide.
  • 15. An optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a refracting concentrator element for collecting and repositioning light; andb) an associated redirecting element which is associated with and separate from the concentrating element for receiving light from the concentrating element wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction and the layer being contiguous between at least a portion of each of the associated redirecting elements;and the optical concentrator further including:a stepped waveguide for receiving the light from the at least one portion of the associated redirecting element which is constructed to reposition the light into the stepped waveguide for accumulation; andan additional optical element coupled to the stepped waveguide that redirects the light from the waveguide towards a light receiver.
  • 16. An optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a concentrating element for collecting and repositioning light; andb) an associated redirecting element which is associated with and separate from the concentrating element for receiving light from the concentrating element, wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction, and the layer being contiguous between at least a portion of each of the associated redirecting elements;the optical concentrator further including a stepped waveguide for receiving the light from the at least one portion of the associated redirecting element which is constructed to reposition the light into the stepped waveguide for accumulation;the above elements being constructed in a cross-section, the cross-section then being extruded to form the optical concentrator.
  • 17. An optical concentrator, comprising: a plurality of optical elements disposed adjacent each other with each of the plurality of optical elements including:a) a concentrating element for collecting and repositioning light, wherein the light is repositioned along one axis of the concentrating element; andb) an associated redirecting element which is associated with and separate from the concentrating element for receiving light from the concentrating element, wherein the concentrating element of each of the plurality of optical elements is separated from at least one portion of the associated redirecting element by a layer within which the light does not undergo a repositioning change of direction, and the layer being contiguous between at least a portion of each of the associated redirecting elementsthe optical concentrator further including a stepped waveguide for receiving the light from the at least one portion of the associated redirecting element which is constructed to reposition the light into the stepped waveguide for accumulation.
CROSS-REFERENCE TO RELATED PATENT APPLICATIONS

This application is continuation application and claims priority to U.S. patent application Ser. No. 12/207,346 now U.S. Pat. No. 7,664,350, filed Sep. 9, 2008, which claims priority to U.S. patent application Ser. No. 11/852,854 now U.S. Pat. No. 7,672,549, filed Sep. 10, 2007, incorporated herein by reference in its entirety.

US Referenced Citations (153)
Number Name Date Kind
705778 McCabe Jul 1902 A
3780722 Swet Dec 1973 A
4029519 Schertz et al. Jun 1977 A
4357486 Blieden et al. Nov 1982 A
4379944 Borden et al. Apr 1983 A
4411490 Daniel Oct 1983 A
4505264 Tremblay Mar 1985 A
4863224 Afian et al. Sep 1989 A
5050946 Hathaway et al. Sep 1991 A
5146354 Plesinger Sep 1992 A
5150960 Redick Sep 1992 A
5237641 Jacobson et al. Aug 1993 A
5253089 Imai Oct 1993 A
5303322 Winston et al. Apr 1994 A
5323477 Lebby et al. Jun 1994 A
5339179 Rudisill et al. Aug 1994 A
5341231 Yamamoto et al. Aug 1994 A
5353075 Conner et al. Oct 1994 A
5359691 Tai et al. Oct 1994 A
5386090 Hofmann Jan 1995 A
5390085 Mari-Roca et al. Feb 1995 A
5390276 Tai et al. Feb 1995 A
5392199 Kashima et al. Feb 1995 A
5396350 Beeson et al. Mar 1995 A
5400224 DuNah et al. Mar 1995 A
5408388 Kobayashi et al. Apr 1995 A
5410454 Murase et al. Apr 1995 A
5418384 Yamana et al. May 1995 A
5420761 DuNah et al. May 1995 A
5428468 Zimmerman et al. Jun 1995 A
5432876 Appeldorn et al. Jul 1995 A
5438484 Kanda et al. Aug 1995 A
5440197 Gleckman Aug 1995 A
5455882 Veligdan Oct 1995 A
5467417 Nakamura et al. Nov 1995 A
5477239 Busch et al. Dec 1995 A
5479275 Abileah Dec 1995 A
5485291 Qiao et al. Jan 1996 A
5485354 Ciupke et al. Jan 1996 A
5499165 Holmes, Jr. Mar 1996 A
5506929 Tai et al. Apr 1996 A
5521725 Beeson et al. May 1996 A
5528709 Koike et al. Jun 1996 A
5528720 Winston et al. Jun 1996 A
5542017 Koike Jul 1996 A
5555329 Kuper et al. Sep 1996 A
5579134 Lengyel Nov 1996 A
5580932 Koike Dec 1996 A
5581683 Bertignoll et al. Dec 1996 A
5594830 Winston et al. Jan 1997 A
5598281 Zimmerman et al. Jan 1997 A
5608837 Tai et al. Mar 1997 A
5621833 Lau et al. Apr 1997 A
5627926 Nakamura et al. May 1997 A
5631994 Appeldorn et al. May 1997 A
5640483 Lin Jun 1997 A
5647655 Kashima et al. Jul 1997 A
5648858 Shibata et al. Jul 1997 A
5659643 Appeldorn et al. Aug 1997 A
5664862 Redmond et al. Sep 1997 A
5664873 Kanda et al. Sep 1997 A
5667762 Fukushima et al. Sep 1997 A
5668913 Tai et al. Sep 1997 A
5671994 Tai et al. Sep 1997 A
5673128 Ohta et al. Sep 1997 A
5684354 Gleckman Nov 1997 A
5692066 Lee et al. Nov 1997 A
5704703 Yamada et al. Jan 1998 A
5710793 Greenberg Jan 1998 A
5806955 Parkyn, Jr. et al. Sep 1998 A
5828427 Faris Oct 1998 A
5835661 Tai et al. Nov 1998 A
5838403 Jannson et al. Nov 1998 A
5854872 Tai Dec 1998 A
5870156 Heembrock Feb 1999 A
5877874 Rosenberg Mar 1999 A
5892325 Gleckman Apr 1999 A
5905583 Kawai et al. May 1999 A
5905826 Benson, Jr. et al. May 1999 A
5914760 Daiku Jun 1999 A
5926601 Tai et al. Jul 1999 A
5977478 Hibino et al. Nov 1999 A
5982540 Koike et al. Nov 1999 A
5993020 Koike Nov 1999 A
6002829 Winston et al. Dec 1999 A
6005343 Rakhimov et al. Dec 1999 A
6007209 Pelka Dec 1999 A
6021007 Murtha Feb 2000 A
6043591 Gleckman Mar 2000 A
6072551 Jannson et al. Jun 2000 A
6104447 Faris Aug 2000 A
6108059 Yang Aug 2000 A
6111622 Abileah Aug 2000 A
6123431 Teragaki et al. Sep 2000 A
6129439 Hou et al. Oct 2000 A
6134092 Pelka et al. Oct 2000 A
6151089 Yang et al. Nov 2000 A
6164799 Hirmer et al. Dec 2000 A
6172809 Koike et al. Jan 2001 B1
6222598 Hiyama et al. Apr 2001 B1
6234656 Hosseini et al. May 2001 B1
6252155 Ortabasi Jun 2001 B1
6266108 Bao et al. Jul 2001 B1
6313892 Gleckman Nov 2001 B2
6335999 Winston et al. Jan 2002 B1
6347874 Boyd et al. Feb 2002 B1
6351594 Nakamura et al. Feb 2002 B1
6379016 Boyd et al. Apr 2002 B1
6409356 Nishimura Jun 2002 B1
6428198 Saccomanno et al. Aug 2002 B1
6440769 Peumans et al. Aug 2002 B2
6473554 Pelka et al. Oct 2002 B1
6476312 Barnham Nov 2002 B1
6496237 Gleckman Dec 2002 B1
6497939 Obuchi et al. Dec 2002 B1
6512600 Kawai et al. Jan 2003 B1
6576887 Whitney et al. Jun 2003 B2
6592234 Epstein et al. Jul 2003 B2
6612709 Yamada et al. Sep 2003 B2
6623132 Lekson et al. Sep 2003 B2
6639349 Bahadur Oct 2003 B1
6644823 Egawa et al. Nov 2003 B2
6647199 Pelka et al. Nov 2003 B1
6671452 Winston et al. Dec 2003 B2
6730840 Sasaoka et al. May 2004 B2
6738051 Boyd et al. May 2004 B2
6752504 Lee et al. Jun 2004 B2
6755545 Lee Jun 2004 B2
6796700 Kraft Sep 2004 B2
6828007 Obuchi et al. Dec 2004 B2
6842571 Kramer et al. Jan 2005 B2
6851815 Lee Feb 2005 B2
6879354 Sawayama et al. Apr 2005 B1
6948838 Kunstler Sep 2005 B2
6957904 Randall Oct 2005 B2
6966661 Read Nov 2005 B2
6966684 Sommers et al. Nov 2005 B2
6976778 Kamijima Dec 2005 B2
6976779 Ohtsuki et al. Dec 2005 B2
6986660 Kumar et al. Jan 2006 B2
6992733 Klein Jan 2006 B1
6993242 Winston et al. Jan 2006 B2
7018085 Lee et al. Mar 2006 B2
7046907 Miyashita May 2006 B2
7063449 Ward Jun 2006 B2
7286296 Chaves et al. Oct 2007 B2
7664350 Ghosh et al. Feb 2010 B2
7672549 Ghosh et al. Mar 2010 B2
20060174867 Schaafsma Aug 2006 A1
20080202500 Hodges et al. Aug 2008 A1
20080271776 Morgan Nov 2008 A1
20090064993 Ghosh et al. Mar 2009 A1
20090067784 Ghosh et al. Mar 2009 A1
Foreign Referenced Citations (4)
Number Date Country
2001-127331 May 2001 JP
2003-234484 Aug 2003 JP
1020010022006 Mar 2001 KR
WO 2006085339 Aug 2006 WO
Related Publications (1)
Number Date Country
20100142891 A1 Jun 2010 US
Continuations (1)
Number Date Country
Parent 12207346 Sep 2008 US
Child 12705434 US
Continuation in Parts (1)
Number Date Country
Parent 11852854 Sep 2007 US
Child 12207346 US