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Numerical study on unsteady film cooling performance under the mainstream swing condition

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Abstract

Significant unsteady film cooling performance of a turbine shroud can be found under the periodic disturbance of rotor blades. The mainstream flow in film cooling on a turbine shroud is simplified as the periodic swing based on the alternate appearance of the cascade passage flow and the blade tip clearance flow. Three-dimensional unsteady numerical simulation was employed to analyze the film cooling effectiveness with a single cylindrical hole injection at mainstream swing frequencies of 100, 160 and 220 Hz, and at blowing ratios of 0.5, 0.8, 1.1 and 1.4, respectively. A steady simulation was also carried out as a comparison. The results show that mainstream swing provides instantaneous film spots. It is a novel phenomenon in film cooling. Spanwise coverage of film was more uniform compared with the steady case. There are considerable differences of film cooling effectiveness under the various mainstream swing frequencies. A larger swing frequency results in higher spanwise averaged time-averaged film cooling effectiveness.

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Abbreviations

D:

Diameter of the cylindrical hole, m

U :

Mainstream velocity, m/s

T:

Temperature, K

t:

Time, s

X:

Streamwise coordinate, m

Y:

Vertical coordinate, m

Z:

Spanwise coordinate, m

ρ :

Density, kg/m3

μ :

Dynamic viscosity, kg/(m×s)

p:

Pressure at local location of the cooled surface, Pa

p*:

Total pressure at inlet of the mainstream, Pa

f:

Swing frequency of the mainstream inlet velocity, Hz

A:

Area of a grid, m2

m:

The number of time steps in a period

n:

The number of spanwise grids

M:

Blowing ratio, (ρcUc)/(ρU)

η :

Film cooling effectiveness, (T - Taw)/(T- Tc)

η ave :

Spanwise averaged film cooling effectiveness, \(\sum\limits_{i = 1}^n {A_i\eta_i} /\sum\limits_{i = 1}^n {A_i}\)

η ta :

Time-averaged film cooling effectiveness, \(\sum\limits_{j = 1}^m {\eta_j}/m\)

η tave :

Spanwise averaged time-averaged film cooling effectiveness, \(\sum\limits_{J = 1}^m {\sum\limits_{i = 1}^n {A_{ij}} \eta_{ij}} /\sum\limits_{i = 1}^m {\sum\limits_{i = 1}^n {A_{ij}}} \)

κ :

Enhancement factor, (ηtave_f - ηtave_0)/ηtave_0)

θ :

Nondimensional excess temperature, (TreTc) / (TTc)

S r :

Strouhal number, Df/U

R e :

Reynolds number, ρUD/μ

Φ:

Viscous dissipated energy

Cp:

Pressure coefficient, (p* - p)/(1 / 2 ρU2)

aw:

Adiabatic wall

c :

Coolant

∞:

Mainstream

ave:

Spanwise averaged

tave:

Spanwise averaged time-averaged

ta:

Time-averaged

tave_f:

Spanwise time-averaged of various swing frequencies

tave_0:

Spanwise time-averaged without swing frequencies

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Acknowledgments

This study was supported by the National Natural Science Foundation of China (Grant No. 51406124).

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Correspondence to Wei Zhang.

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Recommended by Associate Editor Jaeseon Lee

Wei Zhang received her Ph.D. from School of Propulsion and Energy, Northwestern Polytechnical University, China. Her research interests include heat transfer and film cooling in space propulsion.

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Zhang, W., Zhu, Hr., Yu, Qp. et al. Numerical study on unsteady film cooling performance under the mainstream swing condition. J Mech Sci Technol 33, 5527–5536 (2019). https://doi.org/10.1007/s12206-019-1046-y

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  • DOI: https://doi.org/10.1007/s12206-019-1046-y

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