Heat transfer and fluid dynamics of offset unsubmerged axial and tangential jets impinging on a confined heated rotating disk

This study numerically investigates offset unsubmerged axial and tangential jets impingement on a confined heated rotating disk for electric motor cooling applications. The motor's rotor and stator are modeled as rotating and stationary solid regions, respectively. The multi-phase flow and heat transfer characteristics are analyzed over a range of rotational Reynolds numbers from 1 × 10 5 to 3.7 × 10 6 and jet Reynolds numbers ranging from 4.5 × 10 2 to 7.3 × 10 3 in a confined space. The jet nozzle diameter is 1.5 mm with the jet location fixed at an offset of 70 % of the disk radius. For axial and tangential jets, the ratio of jet impingement distance to nozzle diameter is held constant at 12 and 14.7, respectively. The Volume of Fluid method and a moving mesh rotation model are used to simulate the two-phase flow dynamics. The results show that axial jets achieve effective rotor cooling at a mid-range rotational Reynolds number of 2 × 10 6 and a jet Reynolds number of 7.3 × 10 3 but struggle to cool the stator due to limited oil distribution. Axial jet efficiency improves with higher jet Reynolds numbers; however, performance reduces at extreme rotational speeds, as oil contact with critical areas is reduced. Axial jets are thus most suitable for high rotor heat loads and oil flow rates, as their direct impingement enhances cooling effectiveness. In contrast, tangential jets rely heavily on an optimal velocity ratio between jet exit velocity and rotor speed to achieve efficient cooling. At rotational Reynolds number of 6.1 × 10 5 , tangential jets deliver superior heat transfer and temperature uniformity with a lower jet Reynolds number of 3.7 × 10 3 and an ideal velocity ratio of 1, which promotes oil-air mixing and helical impingement. Tangential jets also exhibit up to 23 % lower drag losses at rotational Reynolds number of 6.1 × 10 5 , and maintain lower pressure losses than axial jets, with an 15 % reduction at rotational Reynolds number of 3.7 × 10 6 due to better alignment with the rotating air. Overall, tangential jets are more efficient for lower flow rates and stator-focused cooling, while a mid-range rotational Reynolds number of 2 × 10 6 optimally balances oil distribution and cooling efficiency for both jet types.

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Publication Details

Journal
International Journal of Thermal Sciences
Published
2025-05-10
DOI
https://doi.org/10.1016/j.ijthermalsci.2025.109984
Citations
3
Primary Topic
Heat Transfer Mechanisms
Type
article
Field-Weighted Citation Impact
2.14

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article

Heat transfer and fluid dynamics of offset unsubmerged axial and tangential jets impinging on a confined heated rotating disk

Ram Balachandar, Zia Ud Din Taj, Majed Etemadi, R. M. Barron et al.
3 citations
International Journal of Thermal Sciences
Heat Transfer Mechanisms
2.14
article

Heat transfer and fluid dynamics of offset unsubmerged axial and tangential jets impinging on a confined heated rotating disk

Ram Balachandar, Zia Ud Din Taj, Majed Etemadi, R. M. Barron, Ashkan Nejati, K. Lakshmi Varaha Iyer
article en
3 citations

Abstract

This study numerically investigates offset unsubmerged axial and tangential jets impingement on a confined heated rotating disk for electric motor cooling applications. The motor's rotor and stator are modeled as rotating and stationary solid regions, respectively. The multi-phase flow and heat transfer characteristics are analyzed over a range of rotational Reynolds numbers from 1 × 10 5 to 3.7 × 10 6 and jet Reynolds numbers ranging from 4.5 × 10 2 to 7.3 × 10 3 in a confined space. The jet nozzle diameter is 1.5 mm with the jet location fixed at an offset of 70 % of the disk radius. For axial and tangential jets, the ratio of jet impingement distance to nozzle diameter is held constant at 12 and 14.7, respectively. The Volume of Fluid method and a moving mesh rotation model are used to simulate the two-phase flow dynamics. The results show that axial jets achieve effective rotor cooling at a mid-range rotational Reynolds number of 2 × 10 6 and a jet Reynolds number of 7.3 × 10 3 but struggle to cool the stator due to limited oil distribution. Axial jet efficiency improves with higher jet Reynolds numbers; however, performance reduces at extreme rotational speeds, as oil contact with critical areas is reduced. Axial jets are thus most suitable for high rotor heat loads and oil flow rates, as their direct impingement enhances cooling effectiveness. In contrast, tangential jets rely heavily on an optimal velocity ratio between jet exit velocity and rotor speed to achieve efficient cooling. At rotational Reynolds number of 6.1 × 10 5 , tangential jets deliver superior heat transfer and temperature uniformity with a lower jet Reynolds number of 3.7 × 10 3 and an ideal velocity ratio of 1, which promotes oil-air mixing and helical impingement. Tangential jets also exhibit up to 23 % lower drag losses at rotational Reynolds number of 6.1 × 10 5 , and maintain lower pressure losses than axial jets, with an 15 % reduction at rotational Reynolds number of 3.7 × 10 6 due to better alignment with the rotating air. Overall, tangential jets are more efficient for lower flow rates and stator-focused cooling, while a mid-range rotational Reynolds number of 2 × 10 6 optimally balances oil distribution and cooling efficiency for both jet types.

International Journal of Thermal SciencesVol. 215
Magna International (United States) (US), University of Windsor (CA)
Natural Sciences and Engineering Research Council of Canada
Openalex Percentile: Top 14%
Heat Transfer Mechanisms
2.14
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