Solar Energy Perspectives - IEA
Solar Energy Perspectives - IEA
Solar Energy Perspectives - IEA
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<strong>Solar</strong> <strong>Energy</strong> <strong>Perspectives</strong>: <strong>Solar</strong> thermal electricity<br />
The high concentrating ratio (hundreds of suns) of the tower concept achieves high<br />
temperatures – 565° for molten salts, 550°C for the steam – thereby increasing the<br />
efficiency at which heat is converted into electricity. Improved efficiency also means<br />
a lower cooling load, thus reducing water consumption in plants in arid areas. It would<br />
also reduce the performance penalty of dry cooling. In addition, the concept is highly<br />
flexible; designers can choose from a wide variety of heliostats, receivers, transfer fluids<br />
and power blocks (some plants have several towers that form one power block). The<br />
potential for cost reduction in thermal storage is particularly impressive. <strong>Solar</strong> towers using<br />
molten salts as HTFs and storage media need three times less storage media than current<br />
trough plants, thanks to the larger temperature difference between the hot and cold molten<br />
salts.<br />
The possibilities of even higher temperatures should be explored using different receiver<br />
technologies. One option is supercritical steam cycles, such as those used in modern coalfired<br />
power plants, which reach overall efficiencies of 42 to 46% with supercritical and ultrasupercritical<br />
designs (thermal-to-electric efficiencies of 45% to 50%). Typically, modern<br />
coal-fired power plants use steam at up to 620 °C and 24 MPa to 30 MPa, but by 2020 could<br />
reach 700 °C and 35 MPa, using nickel-based alloys to achieve overall efficiencies<br />
approaching 50%. The application of this technology to solar towers, however, will require<br />
some adaptation.<br />
Direct steam generation (DSG) will pose particular challenges in synchronising solar fields<br />
with receivers and supercritical steam turbines. A continuous management of solar<br />
collectors will be needed to avoid problems during start-up and variations caused by<br />
clouds and at sunset. <strong>Solar</strong> towers with high-temperature HTFs and storage may prove<br />
more capable of fulfilling these requirements, as they disconnect solar heat collection and<br />
power generation. Superheating with some fuel, or full hybridisation in solar-gas or solarcoal<br />
plants (see below) could also help address these challenges. <strong>Solar</strong> towers would need<br />
to be paired to fuel each single supercritical turbine, whose minimum electric capacity<br />
today is 400 MW.<br />
High-temperature tower concepts also include atmospheric air as the HTF (tested in<br />
Germany with the Jülich solar tower project) with solid material storage. <strong>Solar</strong>-to-electricity<br />
efficiencies of up to about 25% can be delivered by such towers, but it is not yet clear if<br />
the gain in efficiency may compensate for the cost and complication of the cycle.<br />
Molten salts decompose at higher temperatures, while corrosion limits the temperatures<br />
of steam turbines. Higher temperatures and efficiencies could rest on the use of fluorideliquid<br />
salts as HTFs up to temperatures of 700°C to 850°C, with closed-loop multi-reheat<br />
Brayton cycles using helium or nitrogen, which have initially been developed for hightemperature<br />
nuclear reactors (Figure 8.3). On top of higher plant efficiency, such power<br />
systems operate at relatively high pressure and power densities that implies smaller<br />
equipment than for steam cycles with their large low-pressure low-power-density<br />
turbines, so they could cost less. The preferred heat-storage medium in this case would<br />
be graphite.<br />
<strong>Solar</strong>-based open Brayton cycles offer a completely different way of exploiting the higher<br />
working temperatures that towers can achieve. Pressurised air would be heated in the solar<br />
receivers, and then sent directly to a gas turbine, at a temperature exceeding 800°C. The<br />
pressurised air can be further heated in a gas fired combustion chamber to reach 1300°C,<br />
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© OECD/<strong>IEA</strong>, 2011