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Solar energy construction 


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Solar energy: How does it work? 

What is the principle behind solar energy cells and how does it work? What type of system do I need? I live in a usually cloudy area, can I still use solar energy? 

These and other questions are answered by the following sites.

 

 

B. Huebner  
How do solar panels work?

Phil Fear 
How do I make my own solar generator?

Photovoltaic Power 
How much is it and what do I need?
 

University of Berlin, Germany 
The six types of solar cell. 

University of New South Wales 
What are solar cells? 

   
   
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radiation from the Sun capable of producing heat, causing chemical reactions, or generating electricity. The Sun is an extremely powerful energy source, and solar radiation is by far the largest source of energy received by the Earth, but its intensity at the Earth's surface is actually quite low. This is partly because the Earth's atmosphere and its clouds absorb or scatter as much as 54 percent of all incoming sunlight. Despite this, in the 20th century solar energy became increasingly attractive as an energy source owing to its inexhaustible supply and its nonpolluting character, which are in stark contrast to such fossil-fuel sources as coal, oil, and natural gas.

The sunlight that reaches the ground consists of nearly 50 percent visible light, 45 percent infrared radiation, and smaller amounts of ultraviolet light and other forms of electromagnetic radiation. This radiation can be converted either into thermal energy (heat) or into electrical energy, though the former is easier to accomplish. Two main types of devices are used to capture solar energy and convert it to thermal energy: flat-plate collectors and concentrating collectors. Because the intensity of solar radiation at the Earth's surface is so low, both types of collectors must be large in area. Even in sunny parts of the world's temperate regions, for instance, a collector must have a surface area of about 430 square feet (40 square m) to gather enough energy to serve one person for one day.

The most widely used flat-plate collectors consist of a blackened metal plate, covered with one or two sheets of glass, that is heated by the sunlight falling on it. This heat is then transferred to air or to water, called carrier fluids, that flows past the back of the plate. The heat may be used directly or it may be transferred to another medium for storage. Flat-plate collectors are commonly used for hot-water heating and house heating. The storage of heat for use at night or during cloudy days is commonly accomplished by using insulated tanks to store the water heated during sunny periods. Such a system can supply a home with hot water drawn from the storage tank or, with the warmed water flowing through tubes in floors and ceilings, it can provide space heating. Flat-plate collectors typically heat carrier fluids to temperatures ranging from 66 to 93 C (150 to 200 F). The efficiency of such collectors (i.e., the proportion of the energy received that they convert into usable energy) ranges from 20 to 80 percent, depending on the design of the collector. (See also solar heating.)

When higher temperatures are needed, a concentrating, or focusing, collector is used. These devices reflect sunlight from a wide area and concentrate it onto a small blackened receiver, thereby considerably increasing the light's intensity in order to produce high temperatures. The arrays of carefully aligned mirrors used in these so-called solar furnaces can focus enough sunlight to heat a target to temperatures of 2,000 C (3,600 F) or more. This heat can be used to study the properties of materials at high temperatures, or it can be used to operate a boiler, which in turn generates steam for a steam-turbine-electric-generator power plant. The solar furnace has become an important tool in high-temperature research. For producing steam, the movable mirrors are so arranged as to concentrate large amounts of solar radiation upon blackened pipes through which water is circulated and thereby heated.

Solar radiation may be converted directly into electricity by photovoltaic cells. In such cells, a small electrical voltage is generated when light strikes the junction between a metal and a semiconductor (such as silicon) or a junction between two different semiconductors. (See photovoltaic effect.) The voltage generated from a single photovoltaic cell is typically only a fraction of a volt. By connecting large numbers of individual cells together, however, as in modern solar batteries, more than one kilowatt of electric power can be generated. The energy efficiency of most present-day photovoltaic cells is only about 7 to 11 percent; i.e., only that fraction of the radiant energy received is converted to electrical energy. And since the intensity of solar radiation is low to begin with, huge and costly assemblies of such cells are required to produce even moderate amounts of power. Consequently, photovoltaic cells that operate on solar light have so far been used mainly for low-power applications--as power sources for calculators and watches, for example. Larger units have been used to provide power for weather and communications satellites.

Solar energy is also used on a small scale for other purposes besides those described heretofore. In some countries, for instance, specially designed solar ovens are employed for cooking, and solar energy is used to produce salt from seawater by evaporation.

The potential for solar energy is enormous, since each day the Earth receives in the form of solar energy about 200,000 times the total world electrical-generating capacity. Unfortunately, though solar energy itself is free, the high cost of its collection, conversion, and storage has limited its exploitation.

 
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Structure and principles of operation

The basic structure of a typical solar cell, whether it is used in a central power station, a satellite, or a calculator, is shown in Figure 1

 
Figure 1: A commonly used solar-cell structure. In many such cells, the absorber layer and...

. As may be seen, light enters the device through a layer of material called the antireflection layer. The function of this layer is to trap the light falling on the solar cell and to promote the transmission of this light into the energy-conversion layers below. Such materials as silicon oxides or titanium dioxide are employed as the antireflection layer in solar cells. The photovoltaic effect, which causes the cell to convert light directly into electrical energy, occurs in the three energy-conversion layers below the antireflection layer. The first of these three layers necessary for energy conversion in a solar cell is the top junction layer in Figure 1 . The next layer in the structure is the core of the device; this is the absorber layer. The last of the energy-conversion layers is the back junction layer.

 

As may be seen from Figure 1 , there are two additional layers that must be present in a solar cell. These are the electrical contact layers. There must obviously be two such layers to allow electric current to flow out of and into the cell. The electrical contact layer on the face of the cell where light enters is generally present in some grid pattern and is composed of a good conductor such as a metal. The grid pattern does not cover the entire face of the cell since grid materials, though good electrical conductors, are generally not transparent to light. Hence, the grid pattern must be widely spaced to allow light to enter the solar cell but not to the extent that the electrical contact layer will have difficulty collecting the current produced by the cell. The back electrical contact layer has no such diametrically opposed restrictions. It need simply function as an electrical contact and thus covers the entire back surface of the cell structure. Because the back layer must be a very good electrical conductor, it is always made of metal.

It is a fundamental fact of nature that, whenever different materials are placed in contact, an electric field exists at the interface, or junction, between these materials. The role of the junction layers in Figure 1 is to establish this electric field. The field created in the solar cell by the different junction-forming materials is termed the built-in electric field. An electric field is needed in a solar cell because it exerts a force on electrons. If electrons are not attached to specific atoms but are free to roam about in a material, they always will move in a direction dictated by the electric field. This movement constitutes an electric current.

The electric field set up by the junction-forming layers of the solar cell causes a current to flow when there are free electrons present in the top junction-forming layer, the absorber layer, and the back junction-forming layer. When light falls on the cell, free electrons occur as a result of the interaction of the light with the absorber layer. The special attribute of this cell layer is that it absorbs light by changing the energy and state (or condition) of some of the electrons in the material. When light is absorbed in the materials, the energy of an electron increases from the so-called ground state energy to an excited energy state. In the excited state, electrons are no longer associated with specific atoms in the absorber, but they are, instead, free to move.

In summary, the absorption of light in the absorber material of a solar cell results in energetic, free electrons that move in the direction forced on them by the built-in electric field. These energetic electrons of the induced current are then collected by the electrical contact layers for use in an external circuit where they can do useful work.

Since most of the energy in sunlight or indoor light is in visible light, a solar-cell absorber should be a strong absorber of electromagnetic radiation in that range of wavelengths. Materials that absorb the visible light of sunlight or of indoor light by producing excited free electrons belong to a class of substances known as semiconductor materials. Semiconductors can absorb all incident visible light in thicknesses of about one-hundredth of a centimetre or less; consequently, the thickness of a solar cell can be of this size. Examples of semiconductor materials employed in solar cells include silicon, gallium arsenide, indium phosphide, and copper indium selenide.

The materials in a solar cell used for the junction-forming layers need only be dissimilar, and, to carry the electric current, they must be conductors. The two junction-forming layers may be different semiconductors or they may be a metal and a semiconductor. Thus, the materials used to construct the various layers of solar cells are essentially the same materials used to produce the diodes and transistors of solid-state electronics and microelectronics (see also electronics: Optoelectronics). Solar cells and microelectronic devices share the same basic technology. In solar-cell fabrication, however, one seeks to construct a large-area device because the power produced is proportional to the illuminated area. In microelectronics the goal is of course to construct devices of very small area to increase the number of circuit components on a single tiny semiconductor chip.

The photovoltaic effect that causes the direct energy conversion in a solar cell is summarized in the schematic of Figure 2

 
Figure 2: Representation of an electron in a solar cell.

. An analogy between an electron in the solar cell and a child at a slide is also presented in this figure. As shown, initially both the electron and the child are in their respective ground states. Next the electron is lifted up to its excited state by consuming energy in the incoming light, just as the child is lifted up to an excited state at the top of the slide by consuming chemical energy stored in his body. In both cases, there is now energy available in the excited state that can be expended. The excited electron is free and moves to the external circuit due to the built-in electric field. It is in this external circuit that the electron will dissipate its excess energy in some device, which in general can be termed a load. The external load is shown here as a simple resistor, but it can be any of a myriad of electrical or electronic devices ranging from motors to radios. Correspondingly, the child moves to the slide because of his desire for excitement. It is on the slide that the child dissipates his excess energy. Finally, when the excess energy is expended, both the electron and the child are back in the ground state where they can, of course, begin the whole process over again. As can be seen from the figure, the motion of the electron, like that of the child, is in one direction. In short, a solar cell produces a direct electric current--namely, one that flows constantly in only a single direction.

 

The photovoltaic process bears certain similarities to photosynthesis in plants by which the energy in light is converted into chemical energy. Since solar cells obviously cannot produce electric power in the dark, part of the energy they develop under light is stored, in many applications, for use when light is not available. One common means of storing this electrical energy is to charge chemical storage batteries. This sequence of converting the energy in light into the energy of excited electrons and then into stored chemical energy is strikingly similar to the process of photosynthesis.

 

   
   

 

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