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to be able to determine the HTF temperature profile along the tube, a simple 1D product has long been produced alongside the collector axis. when the temperature profile is obtained, the tube duration needed to attain the desired HTF temperature within the outlet segment from the receiver tube (550 °C) may be determined in addition. The 1D product exploits the final results on the lumped-parameter product regarding warmth losses correlations with respect to HTF temperature. determine eight illustrates a schematic of your 1D model, incorporating the essential boundary problems. This product solves the constant-point out Electrical power balance equation for the molten salt alongside the receiver axis. As demonstrated in determine eight, the used boundary ailments involve the HTF temperature for the inlet and outlet sections with the receiver tube, mass movement price as well as photo voltaic flux transferred to the HTF.

As a result, to attain the very best Image-thermal performance, an solution need to be taken wherein several selective coatings are positioned alongside the receiver tube based mostly on their own Picture-thermal efficiency at distinct HTF temperature ranges.

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As proven in determine 2, a metallic layer is to begin with coated around the outer surface on the tube, characterised by reduced emissivity and superior reflectivity within the infrared variety. The second layer features a cermet layer composed of ceramic and metallic elements to make certain a high absorptance within the photo voltaic spectral vary. The third layer is surely an anti-reflective layer, placed on the exterior side with the tube.

The reference PTC viewed as for Image-thermal optimization is revealed in determine one. As shown, the receiver tube is composed of a stainless-metal absorber tube, enclosed within a borosilicate glass go over. The absorber tube has the perform of absorbing incident solar radiation and transferring it towards the HTF, and that is a combination of molten salt (sixty%wt.

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on the other hand, this temperature is a little impacted with the mass move charge as it truly is strictly linked to the HTF temperature (see Figure 13). Consequently, variants from the Image-thermal effectiveness with regard for the HTF temperature could well be equivalent for various mass movement costs. As observed in Figure fourteen, to achieve the most Image-thermal performance, two significant HTF temperatures of 436 °C and 517 °C is often determined. Therefore, 3 temperature ranges are made, characterised by three distinctive selective coatings:

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