The present disclosure is directed to an optical concentration system and a concentrator solar energy assembly.
BACKGROUND
Optical concentration systems and concentrator solar energy assemblies are known in the prior art. They can be used to concentrate sunlight onto target areas. In the target areas, highly efficient photovoltaic elements such as solar cells or solar thermal absorber elements can be placed. In the concentration systems as known in the prior art, optical systems are used that are either expensive, laborious to manufacture, lose efficiency due to strongly inhomogeneous illumination, or lose a large portion of the light due to absorption and/or reflection and, therefore, are inefficient.
It is, therefore, an object of the present disclosure to provide an optical concentration system and a concentrator solar energy assembly that is easy to produce and that provides a high yield of concentrated light as well as homogenizes the illumination on the target, i.e., the photovoltaic element.
The solution according to the disclosure, allows at least a part of the light that is directed from the first optical element toward the target area to reach the target area unobstructed. Therefore, the optical concentration system can provide a highly efficient system for transporting light to the target area. The term “light cone,” as used herein, refers to the shape of the light beam after passing the first optical element. Since the first optical element concentrates the incoming light, the resulting light beam tapers toward the target area. The boundaries of the light beam may be shaped as a cone, at least in the space close to the target. It may be noted that, if the first optical element has a square aperture, the light beam may be shaped pyramidal at least in the space close to the first optical element. For the sake of convenience, the light that is directed from the first optical element toward the target area is termed “light cone” in the following disclosure.
The light that is directed from the first optical element toward the target area is homogenized, because the first optical element is a multi-focal element.
The second optical element reflects light to a region of the target area that is outside the center of the target area or to a border region of the target area. It may, therefore, serve as a second homogenizer. The light that is concentrated from the first optical element toward the target area generally has a distribution in which the intensity of the light is the highest in the center of the target area. When the reflected light then superimposes with the light outside the center of the target area, the resulting distribution gets homogenized.
To summarize, the first optical element and the second optical element, which each serve as homogenizers, form a double homogenizing system. This solution leads to a homogeneous illumination of the target area and, at the same time, a negligible loss of light, especially compared to a system that uses a point focus created by the first optical element.
Further, advantageous improvements are described in the dependent claims.
Further advantageous improvements will be described in the following disclosure. The improvements described herein may be combined independently of each other, depending on whether a particular advantage of a particular improvement is needed in a specific application.
According to a first advantageous improvement, the first optical element may be adapted to irradiate an area that exceeds the target area. In this case, it is ensured that the whole target area is illuminated. The portion of light that exceeds the target area can be directed by the second optical element toward the target area. In this case, the majority of the light that is part of the light cone reaches the target area.
In a preferred embodiment, the first optical element is a refractive element, such as a Fresnel lens, in particular, a color-mixing Fresnel lens. However, the disclosure is not restricted to a Fresnel lens. Any other suitable multi-focal optical element may be used. For example, the first optical element may be a total internal reflection element or a mirror.
According to another advantageous embodiment, the first optical element may have a surface with an overall planar shape. The first optical element may be part of an array, for example, a Fresnel lens array.
In order to reflect the majority of light that exceeds the target area, the second optical element may completely surround the target area. It may also be possible that the second optical element only partially surrounds the target area. The second optical element may taper toward the target area and/or may be funnel-shaped.
In the following, embodiments of the invention and its improvements are described in greater detail using an exemplary embodiment and with reference to the figures. As described above, the various features shown in the embodiment may be used independently of each other in specific applications.
In the following figures, elements having the same function and/or the same structure will be referenced by the same reference signs. In the drawings:
In the following, the optical concentration system 1 and the concentrator solar energy assembly 9 are described in an order that follows the path of light that illuminates the optical concentration system 1 along an optical axis O. Incoming light 11 illuminates the first optical element 3. The incoming light 11 is, in general, sunlight, and can, therefore, be seen as a bunch of parallel light rays. Preferably, the first optical element 3 is arranged in a way that the incoming light 11 illuminates it with a normal incidence. This is indicated in
The first optical element 3 is adapted to at least partially focus the incoming light 11 in a way that a light cone 13 or a light beam shaped as a truncated pyramid is formed. The first optical element 3 is shown schematically with a rectangular cross-section. It may have any applicable shape. However, it is preferred that at least the outer surface 15 of the first optical element 3 has an overall planar shape. The planar shape may facilitate cleaning of the first optical element 3 and may allow a compact structural form, especially if several optical concentration systems 1 are combined in order to form an array.
The first optical element 3 may be or include a Fresnel lens. However, other optical elements may also be used, for example, an element that uses total internal reflection. More preferably, the first optical element 3 is or includes a color-mixing multi-focal Fresnel lens.
The light cone 13 illuminates the target area 17, which is shown as a dashed line in
Adjacent to the target area 17, the second optical element 5 is placed. The second optical element 5 preferably completely surrounds the target area 17 circumferentially around the optical axis O. Alternatively, the second optical element 5 may only partially surround the target area 17. The second optical element 5 is preferably shaped as the surface of a truncated cone or a truncated pyramid 30. It may taper toward the target area 17 and may surround the target area 17 with its smaller diameter end 32. The second optical element 5 preferably uses external reflection to reflect light toward the target area 17.
The second optical element 5 is adapted to especially reflect parts of the light cone 13 that would exceed the target area 17 if the second optical element 5 was not present. The second optical element 5 is arranged in a way that the light, which is reflected by it onto the target area 17, is preferably directed onto a region 34 of the target area 17 that is outside of the center 23 of the target area 17 and close to the borders of same. Benefits of this arrangement are described in further detail with respect to
The shape of the light distribution 29 depends on the properties of the first optical element 3. The light distribution 29 can generally be described with a bell-shaped or a Gaussian-like function. In the center 23 of the target area 17, the light intensity has a maximum and it falls with increasing distance from the center 23. For comparison, the target area 17 is indicated in
In contrast to this, the optical concentration system 1 with the second optical element 5 provides an advantageous light distribution 31. The tails 33 of the distribution 29 are reflected by the second optical element 5, mostly onto the region 34 of the target area 17. There, the light may superimpose with light of the distribution 29, which is presented by the region 35 of the distribution 29. The region 35 of the distribution 29 is the light that illuminates the region 34 of the target area 17 and is, therefore, the part of the distribution that is located between the maximum of the distribution 29 and the tails 33. The resulting light distribution 31 has two advantages over the light distribution 29:
First, the light distribution 31 is more homogenous since the decrease toward the limits of the target area 17 is lower than for the distribution 29. Second, the integral of the distribution 29 over the target area 17 and, therefore, the amount of collected light, is larger than for the distribution 29, since the tails 33 now also contribute to the collected light.
1 Optical concentration system
3 First optical element
5 Second optical element
7 Photovoltaic element
9 Concentrator solar energy assembly
11 Incoming light
13 Light cone
15 Outer surface
17 Target area
19 Width of the light cone
21 Width of the target area
23 Center of the target area
25 Opening angle of the second optical element
27 Opening angle of the light cone
29 Light distribution without second optical element
30 Truncated cone
31 Light distribution with second optical element
32 Smaller diameter end of truncated cone
33 Tails of the distribution
34 Region on the target area
35 Region of the light distribution
O Optical axis
Number | Date | Country | Kind |
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102015213395.8 | Jul 2015 | DE | national |
This application is a national phase entry under 35 U.S.C. § 371 of International Patent Application PCT/CA2016/050808, filed Jul. 11, 2016, designating the United States of America and published in English as International Patent Publication WO 2017/008152 A1 on Jan. 19, 2017, which claims the benefit under Article 8 of the Patent Cooperation Treaty to German Patent Application Ser. No. 102015213395.8, filed Jul. 16, 2015.
Filing Document | Filing Date | Country | Kind |
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PCT/CA2016/050808 | 7/11/2016 | WO | 00 |