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Initially, optical investigation on the design of the Linear Fresnel Collector module and the secondary reflector system is carried out.
We report the development of a solar thermal collector module based on our proposed design (Ratismith et.al., 2014) of a large acceptance-angle multiple-parabolic trough which surrounds a standard evacuated cylindrical tube containing a planar absorber plate.
For a 200 m long collector module operated between 300 and 500 °C, the isentropic pumping power required to pump the HTF through the receiver is between 11 and 17 kW.
The beams were collected on a multi collector module with eight movable and one fixed Faraday cup displaying a maximum relative mass range of 17%.
For example, we can think of some instances of the Collector module working together for processing a high volume of events.
The available solar beam irradiation in the collector module is the product of its aperture area (A a) and of the direct beam solar irradiation (G b), as Eq. 1 shows [7, 9]: Q_{text{s}} = A_{text{a}} cdot G_{text{b}}.
Similar(51)
The plant design consists of 16 numbers of solar collector modules in a loop.
It is sufficient to use a single axis tracking of the sun and thus long collector modules are produced.
The final results proved that 1050 collector modules lead to 0.3389 kg/s natural gas consumption and to electricity production equal to 14.81 MWel.
Among them, the development of large, all plastic, innovative design, low cost collector modules suitable for mass production is one of the most promising, which will eventually lead to a drastic reduction of the solar collector subsystem cost.
We propose fixed (non-tracking) configurations of solar light collector modules which are designed to operate efficiently throughout the day, i.e. for varying incident angles of direct sunlight, and in conditions of diffuse solar irradiation.
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