Assessing the efficacy of flat-plate solar collectors using nanofluids in the climatic context of Kirkuk city, Iraq

Adnan M. Hussein; Hussein Hayder Mohammed Ali; Zahraa Ali

doi:10.14311/AP.2024.64.0025

Authors

Adnan M. Hussein Northern Technical University, Technical college of Engineering, 36001 Kirkuk, Iraq
Hussein Hayder Mohammed Ali Northern Technical University, Technical college of Engineering, 36001 Kirkuk, Iraq
Zahraa Ali Northern Technical University, Technical college of Engineering, 36001 Kirkuk, Iraq

DOI:

https://doi.org/10.14311/AP.2024.64.0025

Keywords:

nanofluids, flat-plate solar collectors, solar energy, Nusselt number, Reynolds number

Abstract

Solar energy is a key renewable energy source. Research and development have focused on enhancing the heat transfer coefficient, heat gain, and practical efficiency of solar systems. The aim of this study is to evaluate the performance of a flat solar panel collector using a nanofluid under conditions in the city of Kirkuk/Iraq, 35° latitude and 45° longitude, in terms of practical calculation of thermal efficiency. The study included making two solar collectors, one traditional and the other improved using a nanofluid (CuO). The CuO/Water nanofluid was prepared with a volumetric concentration of 0.25 % by mechanical mixing and then ultrasonic mixing to homogenise the particles and eliminate the agglomerations that form inside the fluid. Practical testing was conducted for the two solar collectors, one using distilled water and the other using the nanofluid, during four months (January, February, March, and April) of the year 2023. The experiments revealed that the efficiency progressively improves from 9:00 a.m. to 1:00 p.m. This increase is attributed to solar radiation’s decreasing intensity post 12:00 p.m., while thermal storage and minimised thermal losses continue to contribute. After 2:00 p.m., the efficiency dwindles due to the declining solar radiation intensity. The practical efficiency of a 0.25 % nanofluid (CuO) attains its zenith at a mass flow rate of 0.015 ls⁻¹. Higher mass flow rates enhance heat transfer within fluid-filled tubes. The collector efficiency at this flow rate ranges from 31.66 % in January to 44.44 % in April.

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