This invention relates to an optical system for concentrating sunlight onto a small solar cell and, in particular, to an optical system that employs refraction, rather than mirrors, to concentrate sunlight onto the solar cell.
A concentrated photovoltaic (CPV) system comprises an array of small solar cells (e.g., 1 cm2 or less), where each cell receives light directed to it by an optical system that tracks the sun. The optical system for each cell typically has a light receiving area that is hundreds of times the area of the cell, so that the cell effectively receives energy from hundreds of suns. The alignment of the optical system to the sun (typically within one degree) is very important to maximize the energy impinging on the cell surface and maximize the uniformity of the light distribution over the cell surface.
Such a system differs from less expensive solar cell systems where large panels of single-junction silicon cells are mounted in a fixed position on a rooftop. Such a system is generally referred to as a photovoltaic (PV) system, rather than a CPV system. A PV system has an overall efficiency of about 18%.
A CPV cell typically has a stack of three semiconductor junctions, having the electrical characteristics of three diodes in series. Each junction is formed of a different set of semiconductor materials so as to be sensitive to a different range of wavelengths. The three groups of wavelengths are typically UV, visible, and infrared. Therefore, CPV systems use more of the sun's energy, and fewer CPV cells are needed to achieve the same power output as a PV system. Such CPV systems typically have an overall efficiency of about 28%.
A common optical system for a CPV system comprises a large area Fresnel lens, called a primary optical element (POE), that ideally focuses all of the impinging sunlight onto a receiving surface of a much smaller secondary optical element (SOE). The SOE is directly optically coupled to the cell, such as by a transparent adhesive. The SOE mixes the light from the POE and has the goal of providing uniform illumination of the cell.
The prior art optical systems, especially the SOE portions, suffer from drawbacks such as not achieving uniform light distribution, being very sun-alignment sensitive, being difficult to fabricate due to the robust materials needed to not degrade when subjected to the UV energy of hundreds of suns, and providing stress on the cell since the SOE is typically directly attached to the cell's top surface.
What is needed is a CPV optical system where the SOE provides more uniform distribution of brightness and wavelengths over the cell surface, has a wider light acceptance angle from a rectangular Fresnel lens (the POE), is easy to fabricate, and does not exert significant mechanical stress on the cell.
An optically system for a standard CPV cell, having a top surface area of about 1 cm2 or less, is described. A large rectangular (includes square) Fresnel lens is spaced from an SOE, such as by 10 cm. The Fresnel lens, in one embodiment, is a square having an area of about 625 cm2 (e.g., 25 cm per side).
The SOE has a bottom portion that resembles a truncated inverted pyramid shape. The bottom surface of the SOE has an area that matches the area of the cell and is optically coupled to the top surface of the cell with silicone. The top portion of the SOE comprises a light receiving surface that is made up of a small center square surrounded by rectangular concentric rings, where the inner rings are slightly angled up and the outer rings are at increasingly downward angles as the rings extend to the outer edge of the SOE, so that the top surface generally falls away toward the edges. In one embodiment of an SOE designed for a cell of about 3×3 mm, the size of the inlet top surface is about 9×9 mm and the SOE has a total height of about 14 mm.
Since the Fresnel lens is rectangular, the light impinging on the SOE is generally rectangular and impinges on the top surface of the SOE at various angles. Since the SOE has a rectangular light receiving surface and concentric angled rectangular rings, the SOE top surface efficiently receives the light from the Fresnel lens at the various angles and improves light acceptance uniformity over its surface. The light entering through the rings is refracted downward by the SOE, and the light is totally internally reflected (TIR) by the bottom portion of the SOE so as to mix the incoming light to provide a uniform brightness and wavelength distribution over the cell surface.
Between the sloping top portion and the truncated pyramid shaped bottom portion is a middle portion that has an inward angle connecting the outer square perimeter of the top portion to the narrower bottom portion. The angle of the middle portion is such that light refracted from the outer areas of the top portion does not significantly exit through the angled sides of the middle portion. The middle portion allows the edges of the top portion to overhang the outer edges of the bottom portion to accept more light at wider angles from the POE. This also allows the taper of the bottom portion to be at a steep angle to provide TIR of the light refracted by the top portion.
The designs of the POE and SOE are such that light is not focused at a point or in a plane within the SOE. Rather, the Fresnel rings are designed to distribute their focal areas in a relatively large three-dimensional volume within the SOE to reduce the UV concentration and help enable better mixing of the light. In one embodiment, the Fresnel rings have a cloverleaf shape to distribute the focal areas inside of the SOE, where each Fresnel ring arc has a different focal point. In one embodiment, the focal areas extend along a 6 mm path within the SOE (about half the height of the SOE). Since the UV from many suns is not focused within a small point or area, the SOE material may be silicone instead of glass. Silicone is easy to mold, so the SOE can be made inexpensively with a stringent tolerance.
Since the SOE is silicone, it can be optically coupled to the top surface of the cell using a silicone adhesive. To avoid the cell fully supporting the SOE, the SOE is molded to have an integral support structure connected to the middle portion of the SOE. The support structure may consist of four flat walls that are spaced from the bottom portion of the SOE by an air gap so as not to affect the TIR of the bottom portion. The middle portion is angled such that an insubstantial amount of light is tapped off by the support structure. The bottom surface of the support structure is adhesively affixed to the circuit board (or other substrate) supporting the cell.
In another embodiment of the SOE 18, the top down shape is not square but may be any shape, depending on the shape of the cell and POE. Additionally, the concentric rings on the SOE 18 need not be flat but may be rounded and form a smooth sloping surface.
Other features are also described.
Elements labeled with the same numeral are the same or equivalent.
The combination of the cell 10, board 12, and optical system is a module that is connected together by a housing, frame, or other structure to maintain the proper spacing and alignment.
The angled prisms of the POE 16 direct the sunlight toward the top surface of a secondary optical element (SOE) 18, as shown by rays 20. In one embodiment, the POE 16 is spaced about 10 cm from the top of the SOE 18, and the height of the SOE 18 is about 14 mm.
The top portion 23 of the SOE 18 comprises a flat center area 24 and four square concentric rings 25-28. The inner ring 25 slightly angles upward and rings 26-28 progressively increase in angle downward toward the edge so that each of the rings is generally normal to the light rays impinging on it from the POE 16. There may be more inner or outer rings in an actual embodiment. For example, as shown in
The generally downward slope of the SOE 18 top surface, in conjunction with its relatively wide width, provides a wide acceptance angle of light so the module does not need to be perfectly aligned with the sun. As the module becomes more out of alignment with the sun, more light will impinge upon the outer rings of the SOE 18. Since each quadrant of the SOE 18 is identical, and each quadrant of the POE 16 is identical, there is very uniform light mixing inside the SOE 18.
The light rays 20 are mixed in the bottom portion 34 of the SOE 18, where the light rays 20 reflect off the flat side walls by TIR. The bottom portion 34 has a truncated pyramid shape that extends from the cell surface to the middle portion 36 of the SOE 18.
The focal volume 32 has different cross-sectional shapes along its length since the different rings of the POE 16 create different patterns. For example, as shown in
The SOE 18 can be formed of a thermoset silicone. Thermoset silicone can be easily molded using injection molding or compression molding. In one embodiment, the SOE 18 is molded directly over the board 12 (or other support surface) on which many cells 10 are mounted, so that many SOE's are formed simultaneously. The molding and curing process causes the SOE 18 to be adhered to the cell 10 and board 12 (including adhered to metal pads or conductors, etc.) without any special adhesive step.
The SOE 18 can be easily molded to include the integral support structure 22, shown in
In one embodiment, the flat bottom surface of the bottom portion 34 is affixed to the top of the cell 10 by a silicone adhesive for good optical coupling. Since the SOE 18 is primarily supported by the support structure 22 affixed to the circuit board 12 (or other support structure) the SOE 18 does not mechanically stress the cell 10.
In another embodiment, the support structure 22 is not angled outward but is still separated from the bottom portion 34 by an air gap so as not to affect the TIR of the bottom portion 34. In another embodiment, the support structure 22 is an extension of the top portion 23 rather than connected to the middle portion 36. The support structure need not completely surround the bottom portion 34. Many configurations of the support structure 22 are possible.
In another embodiment of the SOE 18, the top down shape is not square but may be any shape, depending on the optimal shape required for the system, such as depending on the shape of the cell and POE. The shape may also be a non-square rectangular, round, polygonal, or other shape. Additionally, the concentric rings on the SOE 18 need not be flat but may be rounded and form a smooth sloping surface (no separate rings).
The combination of the POE 16 and SOE 18 provides substantially uniform light over the top surface of the cell, where both brightness and wavelengths are uniformly distributed so that the three diode junctions in the cell are fully exposed to the concentrated sunlight for maximum current output.
Having described the invention in detail, those skilled in the art will appreciate that given the present disclosure, modifications may be made to the invention without departing from the spirit and inventive concepts described herein. Therefore, it is not intended that the scope of the invention be limited to the specific embodiments illustrated and described.