This invention is directed to solar energy concentrators, and more particularly on solar energy concentrators which employ an optofluidic system based on electrowetting to deflect incoming sunlight onto photovoltaic (PV) cells.
Much effort is being expended on the quest to efficiently obtain electrical energy from the sun. One current approach involves providing a large array of photovoltaic (PV) cells, which must be mechanically re-oriented throughout the day in order to properly track the incoming sunlight and thereby maximize the array's electrical output. An alternative approach requires that a large array of mirrors be mechanically re-oriented throughout the day in order to properly reflect and concentrate the incoming sunlight onto a receiver. These systems have several drawbacks. PV cells tend to be costly, and thus a large array of such cells may be prohibitively expensive. In addition, both of these approaches require mechanical systems to track the sun; such systems are typically expensive, consume large amounts of power, and can be difficult to maintain.
“High efficiency PV cells”, also known as “concentrated” PV cells (CPVs) can be used to increase the electrical output of a solar energy system. However, CPVs are very expensive and would not be practical for use in a large array.
Solar energy concentrator architectures are presented which overcome the problems identified above, providing tracking of the sun without a mechanical system and enabling sunlight to be easily concentrated on an array of PV cells or CPVs.
Several solar energy concentrator architectures are described, each of which employs an array of electro-optical devices to deflect sunlight onto PV cells. The preferred electro-optical device is a liquid prism module that employs the electrowetting-on-dielectric (EWOD) principle. Each module comprises a container having a plurality of sidewalls, at least one of which includes an electrode layer and a dielectric layer. At least one liquid fills a portion of the container and contacts the electrode-containing sidewalls. When the container is transparent and contains two immiscible fluids, and voltages are applied to the electrode-containing sidewalls, the interface of the two liquids tilts to bend the beam. In other words, the contact angle along the fluid-fluid-solid tri-junction line—and hence the orientation of the fluid-fluid interface—can be actively controlled via electrowetting. When the immiscible fluids have difference refractive indices, the naturally-formed meniscus between the two liquids functions as an optical prism. Without any mechanical moving parts, this dynamic liquid prism allows the concentrator to adaptively track the daily changes in the sun's orbit. The present system eliminates the power consumption, bulky tracking hardware and noise associated with mechanical tracking.
The concentrator's electro-optical devices may be arranged, for example, into a sheet-shaped array, and include a condenser device such as a Fresnel lens to focus the light deflected by the modules onto one or more PV cells—preferably CPVs. Two or more sheet-shaped arrays may be stacked so as to increase the angle with which light can be deflected.
Another possible concentrator architecture requires arranging a plurality of electro-optical devices into a semi-spherical pattern, such that light impinging on the modules is directed onto one or more PV cells or CPVs.
These and other features, aspects, and advantages of the present invention will become better understood with reference to the following drawings, description, and claims.
The detailed description of embodiments of the invention will be made with reference to the accompanying drawings, wherein like numerals designate corresponding parts in the figures.
a is a diagram of a liquid prism module as might be used as part of a solar energy concentrator architecture per the present invention.
b is a diagram illustrating the layers and the operation of a liquid prism module as shown in
Several unique solar energy concentrator architectures are described herein, each of which employs an array of electro-optical devices to deflect sunlight onto PV cells. Any type of electro-optical device capable of deflecting incoming sunlight may be employed, including, for example, a liquid crystal device or a Risley prism. The preferred device is a electro-optical prism that employs the electrowetting-on-dielectric (EWOD) principle. The term “liquid prism module” is used herein to refer to this type of prism, which appears in all of the illustrated embodiments; note, however, that the present solar energy concentrator architectures may also employ other electro-optical device types.
An exemplary embodiment of such a liquid prism module is shown in
Note that a prism as shown in
One possible embodiment of a solar energy concentrator per the present invention is shown in
A sectional view of another possible embodiment of a solar energy concentrator per the present invention is shown in
As previously noted, the present system preferably employs high-efficiency CPV PV cells. Preferred CPV cells employ III-V materials, and are more efficient than traditional silicon-based PV cells (40% vs. 15%-19%). The use of these cells provides a much higher energy yield with less PV material.
The EWOD mechanism employed by the liquid prism modules described herein is used as a surface-tension-control technique. The contact angle change of a liquid by electrowetting is described by Lippman-Young's equation:
cos θ=cos θY+[∈∈0)/(2γd)]V2,
where θ is the contact angle at electric potential V, θY is the contact angle with no electric potential, γ is the liquid-liquid interfacial tension, ∈0 is the permittivity of vacuum, ∈ is the dielectric constant of the insulator layer, and d the thickness of the dielectric insulation layer. Changes in the contact angle can give rise to continuous variations of the fluid-fluid interface curvature and shape. Therefore, the meniscus interface can function as a liquid prism (light deflector) or as a tunable optical lens. Note that if there is only one type of liquid in the cell, γ is the surface tension between the liquid and the vapor (air, gas, etc.) contained within the cell.
As shown in
The present solar energy concentrator can be arranged to continuously align the liquid prism array to deflect sunlight throughout the day so as to maximize electricity generation. This type of design is also lighter and smaller than conventional concentrators, and thus can provide a highly efficient system suitable for rooftop installation.
The present solar energy concentrator can be arranged as a “1-D” embodiment, in which only one independent voltage is applied to a sidewall of each prism module. A “2-D” embodiment which provides 2-D steering can be achieved by providing two independent voltages to respective sidewalls of each cell. A 2-D arrangement enables the concentrator to adaptively track both daily and seasonal changes in the sun's orbit, i.e., dual-axis tracking is provided. The voltages applied to the electrode layers of each module may be approximately equal for every module in an array, in which case the contact angle for each module would be approximately equal and would change in unison. Alternatively, the voltages applied to the electrode layers may be independent for every module in an array. A controller (not shown) would typically be provided to apply the voltages to the electrode layers. An electrowetting-controlled liquid prism module as described herein can provide a wide sun tracking range in excess of ±30°.
A controller is used to apply the necessary voltages to the electrode-containing sidewalls of the liquid prism modules. The voltages may be either DC or AC. The advantages of DC control are low power consumption and fabrication simplicity. However, the dielectric coating on the module walls may be subject to breakdown or permanent polarization when a high DC electric field is applied over an extended period. Using an AC voltage avoids applying a high electric field over a long period to an electrode-containing sidewall, which can significantly increase the reliability and service life of the solar energy concentrator; however, this approach may consume more power and is relatively more complicated. The controller is preferably arranged such that, once programmed, it runs without human intervention—automatically controlling the voltages applied to the sidewalls according to the latitude of the solar energy concentrator and the time of day, so that maximal solar energy is concentrated on the PV cells.
One or more beam steering sheets can be easily scaled to cover a large surface, or form a large energy farm; one possible embodiment is shown in
Another possible solar energy concentrator architecture 90 in accordance with the present invention is illustrated in
Various other modifications and alterations in the structure and method of operation of this invention will be apparent to those skilled in the art without departing from the scope and spirit of the invention. Although the invention has been described in connection with specific preferred embodiments, it should be understood that the invention as claimed should not be unduly limited to such specific embodiments. It is intended that the following claims define the scope of the present invention and that structures and methods within the scope of these claims and their equivalents be covered thereby.
This application claims the benefit of provisional patent application No. 61/446,964 to Wen et al., filed Feb. 25, 2011.
Number | Date | Country | |
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61446964 | Feb 2011 | US |