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Performance enhancement of borehole ground source heat pump using single U-tube heat exchanger with a novel oval cross-section (SUO) and a novel spacer

Sustainable Energy Technologies and Assessments • 2020
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Publication Information
Authors Ahmed A. Serageldin, Yoshitaka Sakata, Takao Katsura, Nagano Katsunori
Keywords Oval U-tubeNovel spacerCFDBHEGSHPBorehole thermal resistanceThermal interference loss rate
Journal Sustainable Energy Technologies and Assessments
Publisher Elsevier
Volume 42
Issue 100805
Pages Not Available
publication.type International
Paper Link Open Link
Supplementary Materials Not Available
Abstract
This study introduces a new, efficient, and cost-effective spacer to maintain the space between the upward and downward U-tube legs of a single U-tube with an oval cross-section. Therefore, short-term and long-term transient numerical simulations were performed to compare the thermal and energy performance of the ground source heat pump system with both a single U-tube with an oval cross-section coupled with a novel spacer, and a conventional single U-tube with a circular cross-section. The impact of using different spacer cross-sections (circular cross-section, oval cross-section, and an oval cross-section with fins, double spacers with circular cross-section), materials, and length on the thermal performance was examined. Finally, a straightforward economic study was implemented to examine the feasibility of utilizing the proposed spacer. A single aluminum spacer with oval and fins cross-section decreases the borehole thermal resistance (Rb) by 25 % and 28 % compared with single U-tube with an oval cross-section and single U-tube with a circular cross-section, respectively. Furthermore, it improves the coefficient of performance (COP) in winter by 9.5 % compared with single U-tube with circular cross-section. Thus, it saves 497 kW·h operating energy. Finally, the economic study shows that the simple payback period for using the single aluminum spacer with oval and fins cross-section of length 50 m is 3.8 y.