1. Numerical analysis of convective heat loss from a cylindrical–hemispherical receiver using a glass cover and an air curtain.
- Author
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Kumar, Kolli Harish, Karmakar, Malay, and Mondal, Bittagopal
- Subjects
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HEAT losses , *NUMERICAL analysis , *FORCED convection , *WIND speed , *PARABOLIC reflectors , *NATURAL heat convection , *DOPPLER effect - Abstract
It is imperative to mitigate the convective heat loss from the receiver to improve the overall efficiency of the parabolic dish concentrator. In this study, the reductions of convective heat loss from the cylindrical‐hemispherical receiver are numerically analyzed and the model was validated by the experimental data from literature. In the first case, the impact of the glass cover on convective heat loss is examined under conditions of both natural and forced convections at various receiver orientations (γ = 0°, 30°, 60°, and 90°). Numerical results clearly demonstrate that the use of a glass cover significantly reduces the intrusion of surrounding air into the receiver cavity which leads to an enhancement of the stagnation zone inside the cavity and, as a consequence, a noticeable reduction in convective heat loss is observed. To perform analysis of the receiver with glass cover under forced convective condition, the wind velocities over the receiver are considered in the range of 1–6 m/s. The maximum reduction of convective heat loss using the glass cover is achieved to be 58.44% with wind velocity of 5 m/s at γ = 60°. In the second case, the influence of air curtain at the receiver aperture under natural convective heat loss conditions is analyzed. The analysis incorporates three variables: receiver orientation (γ = 0°–60°), nozzle width (Lnoz ${L}_{\mathrm{noz}}$ = 0.002–0.004 m), and nozzle outlet velocity (Vnoz ${V}_{\mathrm{noz}}$ = 0.5–3.5 m/s). The results show that the air curtain minimizes the outflow of receiver inside air and results in an improvement in the stagnation zone inside the cavity. The maximum effectiveness of the air curtain is found to be 43.2% at nozzle width of Lnoz ${L}_{\mathrm{noz}}$ = 0.004 m and nozzle velocity of Vnoz ${V}_{\mathrm{noz}}$ = 1.5 m/s at receiver orientation of 60°. It is also noteworthy that the optimal nozzle velocity decreases with the increase of nozzle widths. [ABSTRACT FROM AUTHOR]
- Published
- 2024
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