This invention relates to solar windows configured to generate electricity, especially those using prismatic optics to concentrate impinging solar radiation.
It is well known that solar radiation can be utilized by various methods to produce useable energy. One method involves the use of a photovoltaic cell, which is configured to convert solar radiation to electricity. Solar radiation collectors are typically used to gather sunlight or other radiation and direct it toward a photovoltaic cell. Often, concentrators are provided in order to focus the radiation from an area to a photovoltaic cell which is smaller than the area.
Often, a plurality of photovoltaic cells is provided to form a single module. This module may be formed so as to have characteristics separate from energy production which make it useful as a construction element. For example, the module may allow some light to pass therethrough without being used for energy production. Such a module may be installed in a building and used as a window or skylight.
Typically separation of light rays where a first portion thereof is for energy production and a second portion thereof is used for introducing light into the building is carried out by a window, such as double glazed window having a pair of prisms mounted therein. Such as window is disclosed for example in WO 2010/076796 disclosing a photo-voltaic windows and skylights integrating an array of PV cells within a double glaze cavity, and applying optical elements that direct some or most of the direct light towards the PV cell for electricity production, while allowing diffuse light to penetrate through the window into the building providing natural day light illumination and/or clear view to the outside of the building.
In WO 2010/076796 a prism pair is disclosed for concentrating direct solar radiation onto the PV cells, while allowing diffused light from the surroundings to enter through the solar window, allowing a clear view outside. Manufacturing such optical elements using plastic injection molding techniques is difficult and can get very expensive, since it is challenging to mold high quality flat surfaces in asymmetric parts such as the prism.
According to one aspect of the presently disclosed subject matter, there is provided a window comprising a front pane and one or more prism units each comprising: a primary prism disposed adjacent the front pane and having a primary entrance face and a primary exit face. The primary entrance face is configured to receive light that passes through the front pane. The prism unit further comprising a secondary prism disposed adjacent the primary prism and having a secondary entrance face and a secondary exit face. The secondary entrance face is configured to receive from the primary exit face a second portion of the light. At least one of the entrance and exit faces comprises a light diverging surface which causes divergence of light passing therethrough. At least one of the entrance and exit faces different from the light diverging surface, comprises a light converging surface configured to reduce the divergence.
The window can further comprise an adhesive material disposed between the front pane and the primary entrance face. The adhesive material has a refractive index different from that of the primary entrance face, and the primary entrance face comprises the diverging surface or the converging surface.
Each the prism units can be provided with a PV cell, and the primary exit face can be configured to direct a first portion of the light towards the PV cell. The first portion includes at least light rays reaching the primary exit face in an angel which is larger than the critical angle thereby being totally reflected toward the PV cell.
The prism units can include a plurality of prism units, each configured to form an image of a portion of an object disposed outside the front pane of the window. The prism units is at such relative disposition and having their converging surfaces of such shapes as to ensure that the images form a continuous image of the object.
According to another aspect of the presently disclosed subject matter, there is provided a PV assembly for a double glazed window having a front pane and a rear pane with space therebetween. The assembly comprising at least one PV cell disposed in the space, the PV cell is configured to convert light rays to electrical energy, and one or more prism units. Each of the prism units comprising a primary prism disposed adjacent the front pane and having a primary entrance face and a primary exit face. The primary entrance face is configured to receive light that passes through the front pane, and to direct a first portion of the light towards the PV cell. The prism unit further comprising a secondary prism disposed adjacent the primary prism and having a secondary entrance face and a secondary exit face. The secondary entrance face is configured to receive from the primary exit face a second portion of the light different from the first portion, and the secondary exit face is configured to direct at least the second portion of light toward the rear pane. At least one of the entrance and exit faces comprises a light diverging surface which causes divergence of light passing therethrough, At least one of the entrance and exit faces different from the light diverging surface, comprises a light converging surface configured to reduce the divergence.
The PV cell can include a plurality of PV cell and the prism units can include a plurality of prism units, each configured to form an image of a portion of an object disposed outside the front pane of the window. The prism units can be at such relative disposition and having their converging surfaces of such shapes as to ensure that the images form a continuous image of the object, each one of the prism unit is associated with one of the PV cells.
The diverging surface can be configured to diverge the light in a manner pre-determined prior to the production of the corresponding prism.
The light diverging surface can be a concaved curvature formed in a controlled manner with a predetermined focal length.
The divergence can be determined after the corresponding prism is produced. The light diverging surface is a concaved curvature formed in an uncontrolled manner during the injection process of the primary and secondary prisms.
The light converging surface is a convex surface formed in a controlled manner with a predetermined focal length.
According to another aspect of the presently disclosed subject matter, there is provided a method for forming a PV assembly for a double glazed window having a front pane and a rear pane with space therebetween. The method comprising the step of providing a PV cell for mounting inside the space, the PV cell is configured to convert light rays to electrical energy. The method further comprising forming a primary prism having a primary entrance face and a primary exit face, the primary entrance face being configured to receive light that passes through the front pane, and when deposed in the space to direct a first portion of said light towards said PV cell. The method further comprising the step of forming a secondary prism having a secondary entrance face and a secondary exit face. The secondary entrance face is configured when deposed in the space to receive from the primary exit face a second portion of said light different from the first portion, and the secondary exit face being configured to direct at least the second portion of light toward the rear pane. Determining the light divergence of light passing through the primary prism and secondary prism, and providing at least one of the entrance and exit faces with a light converging surface which is configured to reduce said divergence.
At least one of the entrance and exit faces can be provided with a light diverging surface different from the light converging surface. Determining the light divergence can be carried out in consideration with the refractive index of the adhesive material disposed between the front pane and the primary entrance face.
In order to understand the presently disclosed subject matter and to see how it may be carried out in practice, embodiments will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which:
It is well known to those skilled in the art that obtaining accurate curved surfaces such as the, lens, or the convex surface 28 in an injection process is simpler than obtaining flat surfaces, mainly due to the ability to reach the correct curvature buy doing iterative machining of the mold. Thus, unlike the concaved curvatures 26, which are naturally formed in an uncontrolled manner, when forming a flat surface, the convex surface 28 is formed as a surface having a curvature in a controlled process, and thus can be configured as required so as to mitigate the effect of the light diverging surface of the concaved curvatures 26,
According to the illustrated example, the light diverging surface of the concaved curvatures 26 is formed on the entrance and exit faces 22a and 22b of the primary prism 22, as well as on the entrance face 24a of the secondary prism 24. The convex surface 28 on the other hand is formed on the exit face 24b of the secondary prism 24. In this example, the light rays 21 traveling through the entrance and exit faces 22a and 22b of the primary prism 22, and further through the entrance face 24a of the secondary prism 24, deviate from the original path thereof. Accordingly, the convex surface 28 on the exit face 24b of the second prism 24 is configured to direct the light rays traveling therethrogh substantially in parallel to the optical axis of the prism pair 20, thereby correcting or at least reducing the light divergence caused by the other faces.
It is appreciated that in order to allow a clear image at the exit face 24b of the secondary prism 24 the convex surface 28 does not have to be configured to direct the light rays exiting the prism pair 20 precisely in parallel to the optical axis, and to one another. That is to say that the focus length of the convex surface 28 need not be precisely the sum of the focus lengths of each concave curvature 26. Rather it is sufficient if the light rays are directed in such a way to reduce the light ray divergence, caused by the concaved curvatures 26 of the prism pair. In other words, the exit face 24b of the second prism 24 does not have to be configured in such a way that the total focal length of the prism pair 20 is set to infinity. Rather, the total focal length of the prism pair 20 can be set far enough from the prism pair so as to allow clear image when viewing therethrough.
As shown in
It is appreciated that the convex surface 38 is design as a positive lens having a power which is equal to the sum of the powers of the three adjacent faces. While the three faces act as a negative lens, the face with the convex surface 38 acts as a positive lens, which substantially cancel out the power of the surfaces, and prevent ray divergence. The power of the negative lens formed on the other faces can be determined using accurate measurement techniques. Once the curvature is known the power of the lens can be calculated and then the power of the convex surface 38 can be calculated, and the mold thereof can be configured accordingly.
It is appreciated in accordance with the latter example, the concaved and the convex surfaces 46 and 48 can be formed on any face of the prisms 42 and 44, for example the convex surfaces 48 can be formed on the exit faces 42b and 44b, and the concave surface 46 can be formed entrance face 42a and 44a. Alternatively, one of the prisms can include concaved and the convex surfaces, while the other prism include surfaces with naturally formed concaved curvatures. Accordingly, the concaved and the convex surfaces of one prism are configured to substantially align the light rays passing through the both prisms.
It is further appreciated that the prism unit can be configured to allow light rays passing the through to be directed through the secondary exit face when substantially parallel to one another. Alternatively, the prism unit can be configured to slightly diverge light rays passing therethough, so as to magnify the image created on the exit side thereof. This can be carried out by forming at least one face of the prism unit, with a convex surface as explained above with regards to
It is appreciated that according to the example of
However, a second portion of the light ray which impinge on the exit face 22b in an angle which is smaller than the critical angle travels through the air gap 58 toward the rear pane 52b through the secondary prism 24. The second portion of the light rays may be slightly distorted due to the difference in the refractive indices between the primary prism 22 and the air gap 58. Thus the secondary prism 24 is provided and is configured to bring the second portion of the light rays back substantially to their original path.
As explained in hereinabove with regards to
It is appreciated however, that the primary prism 22 can be coupled to the front pane 52a in such a way that there is substantially no air between the front pane and the primary entrance face 22a so as to preclude reflections on the interface therebetween. This can be carried out for example by gluing the primary prism 22 to the front pane 52a using optical adhesive material 51 which has refractive index other than that of air (r>1), such that can be as close as possible to that of the window and of the prism.
Accordingly, when calculating the necessary curvature of the convex surface 28, the difference in the refractive indices in each boundary must be taken into consideration, so as to calculate the exact effect of each face on the light rays passing therethrough. This can be carried out by using the lens makers' equation (thin lens approximation) may be used:
where f is the focal length, n1 is the refractive index of the lens, n2 is the refractive index of the external material (either air or the optical adhesive), and R1 is the radiuses of the face of the curved surface. The equation can be used to calculate the focal length of the diverging surfaces or the required radios of the converging surface.
Those skilled in the art to which the presently disclosed subject matter pertains will readily appreciate that numerous changes, variations, and modifications can be made without departing from the scope of the invention, mutatis mutandis.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IL2012/050024 | 1/25/2012 | WO | 00 | 7/25/2013 |
Number | Date | Country | |
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61435819 | Jan 2011 | US |