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Conjugated heat transfer characteristics of ribbed-swirl cooling in turbine blade under rotation condition

  • Kun Xiao , Xiandi Zhao , Juan He , Zhaokai Ma EMAIL logo and Zhenping Feng
Published/Copyright: November 25, 2024
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Abstract

Ribbed-swirl cooling performs excellently in enhancing heat transfer, but previous studies were almost conducted in simple circular tubes under static conditions. The influence of actual mainstream flow, heat conduction of blade as well as the rotation effect was ignored. To explore its application potential in a real environment, the thermal performance of swirling cooling after adding annular ribs to its target surface in a real turbine blade was analyzed, and the impacts of centrifugal force along with Coriolis force were also included. From the results, the ribs affected the distribution of nozzle mass flow rate. For nozzles near the blade root, the mass flow rates in ribbed-swirl cooling were smaller than those in smooth-swirl chamber, while near blade tip, those were higher. Besides, the influence of Coriolis force from SS (suction side) to PS (pressure side) on the development of cross-flow and swirl in smooth and ribbed chamber exerted a significant difference. For ribbed-swirl cooling, cross-flow passing through ribs induced flow separation, which was conducted to cross-flow suppression. The combined action of the above two aspects led to an obvious heat transfer advantage of ribbed-swirl cooling. In comparison to smooth-swirl chamber, its blade surface temperature was further reduced to more than 25 K.


Corresponding author: Zhaokai Ma, Ministry of Industry and Information Technology Key Laboratory of Thermal Management and Energy Utilization of Aviation Vehicles, College of Energy and Power Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China, E-mail:

Acknowledgments

The authors would like to acknowledge the financial support from Ministry of Industry and Information Technology Key Laboratory of Thermal Management and Energy Utilization of Aviation Vehicles and Jiangsu Province Provincial department of science and technology (No. BK20241413).

  1. Research ethics: Not applicable.

  2. Informed consent: Not applicable.

  3. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and approved its submission. Kun Xiao: Conceptualization, Data Curation, Formal Analysis, Investigation, Writing – Original Draft, Xiandi Zhao: Methodology, Juan He: Investigation, Writing – Review & Editing, Zhaokai Ma: Funding Acquisition, Writing – Review & Editing, Zhenping Feng: Project Administration.

  4. Use of Large Language Models, AI and Machine Learning Tools: None declared.

  5. Conflict of interest: The author states no conflict of interest.

  6. Research funding: Ministry of Industry and Information Technology Key Laboratory of Thermal Management and Energy Utilization of Aviation Vehicles(No.CEPE2024005), Jiangsu Province Provincial department of science and technology (No. BK20241413).

  7. Data availability: All data generated or analyzed during this study are included in this published article.

Nomenclature

Symbols

Fi

Body force, N

f

Friction factor

H

Height of the jet nozzles, mm

h

Heat transfer coefficient, W/(m2·K)

h r

Height of ribs, mm

L

Length of the swirl chamber, mm

Nu

Nusselt number

N 0

Total internal energy, J

P

Pressure, kPa

PS

Pressure surface

q

Heat flux, W/m2

Re

Reynolds number

S

Area, m2

SS

Suction surface

S ij

Strain rate tensor

T

Temperature, K

t

Time, s

U

Velocity, m/s

W

Width of the jet nozzles, mm

Greek symbols

ρ

Density of gas, kg/m3

μ

Dynamic viscosity, m2/s

λ

Thermal conductively, W/(m·K)

σ ij

Stress tensor

Subscripts

a

Area-averaged

cir

Circumferentially-averaged

In

Inlet

w

Wall

0

Baseline

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Received: 2024-05-23
Accepted: 2024-10-13
Published Online: 2024-11-25
Published in Print: 2025-05-26

© 2024 Walter de Gruyter GmbH, Berlin/Boston

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