1. Field
This disclosure relates to equipment for solar radiation collection.
2. Description of Related Art
Solar radiation collectors try to capture the solar radiation energy that strikes the earth to greatest extent possible. The amount of solar radiation striking any surface area of the earth is a fixed amount per day (without clouds) for any given location and time of year. Conventional flat-panel collectors enlist the use of a metal surface (usually in sheet fashion) with tubes attached to absorb and transfer the thermal energy to a liquid within the tubes, which is then transported elsewhere for use. Conventional parabolic collectors enlist the use of mirrored parabolic surfaces to concentrate the solar radiation onto a metal surface that will absorb and transfer the thermal energy to a liquid or gas within the structure, which is then transported elsewhere for use. Conventional evacuated tube collectors enlist the use of a glass tube that is evacuated of air to eliminate heat loss through convection and radiation. Contained within the tubes, are either a looped tube that contain liquid that is heated or a metal plate that is attached to a hollow tube that contains a liquid that vaporizes and rises to a metal heat exchanger lying within yet another tube that contains a liquid or gas within the tube which is then transported elsewhere for use. Conventional solar radiation collectors typically require that the solar radiation striking the collector in whatever fashion should ultimately pass through a conduit wall or heat exchanger to transfer the heat by means of conduction to a liquid as might be used. Conventional solar collectors are typically limited to a maximum of sixty to seventy percent efficiency.
The flow of thermal energy as required by the second law of thermodynamics goes from a high thermal energy to a lower thermal energy. The law of Heat Conduction or “Fourier's Law”, states that the time rate of heat transfer through a “material” is proportional to the negative gradient in the temperature and to the area at right angles, to that gradient, through which the heat is flowing. In a one-dimensional differential form, Fourier's Law is as follows: q=Q/A=−kdT/dx. The heat transfer or conduction rate of a material is given by: q=−kA (ΔT/L), where, k is the thermal conductivity of the material, L is the length of heat travel through the material (the wall of the conduit), A is the cross-sectional area of material orthogonal to the travel of heat and ΔT is the temperature difference between the two sides, with the final units being Watts per Meter2 or Joules per second making the whole process a time/rate of change situation.
When the intent is to heat a liquid within a conduit to the largest absolute temperature difference between when the liquid enters the system and when the liquid exits, the liquid should have an increased time interval within the system. Increasing the time interval a liquid within the conduit experiences can be accomplished by two means for a given size system (length×width×height): decrease the flow rate of the liquid and/or increase the travel path length as in a serpentine fashion. Many flat panel collectors utilize headers that consolidate the flow from many tubes running across the surface of the collector.
In one aspect, the methods and systems described herein provide a solar radiation collector that improves upon past art and may be incorporated into currently available collector housings.
In another aspect, an apparatus is provided for converting solar radiation into thermal energy via a first and second non-ferrous metal conduit joined in a serpentine configuration by a non-ferrous metal end fitting. In one embodiment, the apparatus is a high performance solar radiation collector converting solar radiation into thermal energy and transferring said thermal energy to a liquid transfer medium flowing through the collector.
In still another aspect, a solar radiation collector employs a plurality of flattened non-ferrous metal conduits that are adjacent to one another. In one embodiment, each of the plurality of flattened non-ferrous metal conduits is located immediately adjacent to another. A plurality of cast molded non-ferrous metal conduit fittings provide for the joining of adjacent flattened non-ferrous metal conduits to cause a reversal in direction of fluid flow to the next adjacent non-ferrous conduit thus creating a serpentine geometry of conduits within the collector housing. Tubes of the same non-ferrous material on the underside and perpendicular hold this collection of conduits and fittings together the lengths of the conduits. In some embodiments, the parts are spray-painted flat black. In other embodiments, a selective chrome-black finish is deposited on the surface of the parts by, for example, electroplating.
In one embodiment, the conduits are made from non-ferrous metal pipes that are flattened. In another embodiment, non-ferrous metal can be extruded into a flattened geometry that forms the conduits. One of ordinary skill in the art should understand the practices that may be used to flatten the pipes or to manufacture by extrusion the flattened conduits.
In some embodiments, the inclusion of the non-ferrous metal end fittings result in improved conduits. In other embodiments, allowing for non-ferrous metal end fittings composed of materials other than copper (such as, and without limitation, aluminum or any non-ferrous material) result in improved conduit.
The foregoing and other objects, aspects, features, and advantages of the disclosure will become more apparent and better understood by referring to the following description taken in conjunction with the accompanying drawings, in which:
A solar radiation collection apparatus utilizes a cast molded non-ferrous metal end fitting to provide for the joining of adjacent flattened non-ferrous metal conduits to facilitate a reversal in direction of fluid flow. The conduit fitting provides for a small offset from the previous and next adjacent conduits thereby maximizing the surface area of the non-ferrous metal flattened conduits exposed to solar radiation within any given enclosure. The serpentine fashion and the thinness of the collector conduits allows for a high absolute temperature difference between when the liquid enters the collector and when the liquid exits the collector thereby making increased heat available for immediate use or stored for use later. In some embodiments, use of a solar radiation collector as described herein may result in a higher efficiency than that provided by conventional collectors.
Referring now to
Referring now to
The non-ferrous metal end fitting 11 can be made by any standard foundry methods such as, without limitation, die-casting, investment casting or sand casting.
Referring now to
In one embodiment, the high performance solar radiation collection apparatus 1 in
In
One of ordinary skill in the art should understand that conventional techniques may be used for the manufacture of the non-ferrous metal flattened conduits. In one embodiment, by way of example, the non-ferrous metal flattened conduits can be made by flattening round conduits to a flat geometry or by extruding non-ferrous metal to the required flattened geometry. In some embodiments, non-ferrous metals that may be used are not limited to copper or aluminum.
This application claims priority from U.S. Provisional Patent Application Ser. No. 61/297,163, filed on Jan. 21, 2010, entitled “High Performance Flat Panel Copper Solar Collector”, which is hereby incorporated by reference.
Number | Date | Country | |
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61297163 | Jan 2010 | US |