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Numerical investigation of nozzle geometry influence on the vortex cooling in an actual gas turbine blade leading edge cooling system

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Abstract

To investigate the nozzle geometry influence on vortex cooling performance in the actual leading edge region, an improved vortex cooling configuration with a coolant chamber is established based on the middle cross section of stage 1 vane blade of GE-E3 high pressure gas turbine. Numerical simulations are conducted to research the effects of nozzle position, nozzle number and nozzle aspect ratio on the flow and heat transfer behavior. Results show that with the introduction of the coolant chamber, the mass flow of nozzles increases gradually from the upstream to the downstream instead of a uniform mass flow distribution. Configurations with nozzles placed at the sides (the vortex cooling) have better cooling performance than with nozzles placed in the middle (the impingement cooling). What’s more, the configuration with nozzles placed along the pressure side has the best comprehensive cooling performance. Due to the irregular blade line, a flow entrainment that is not found in simplified circular configurations is observed on the pressure side weakening the local heat transfer performance. The cooling performance is most sensitive to the nozzle number. As the nozzle number increases, the friction coefficient and heat transfer intensity both decrease. Moreover, as the nozzle aspect ratio increases, the friction coefficient and heat transfer intensity both increases first and then decrease. Results indicate a certain vortex cooling configuration may have the optimal nozzle number and nozzle aspect ratio. For this paper’s configuration, the best nozzle number is 5 and the best nozzle aspect ratio is 4.

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Abbreviations

A:

Width of nozzles (m)

B:

Length of nozzles (m)

D i :

Hydraulic diameter of the inlet (m)

D v :

Hydraulic diameter of the vortex chamber (m)

f :

Friction coefficient, 2ΔPDh/(ρU2L)

f :

Friction coefficient for non-swirling flow in a smooth pipe

h :

Heat transfer coefficient (W/(m2·K))

j :

Thermal performance factor, (Nua/Nu)/( f/f)1/3

L 1 :

Axial distance between adjacent nozzles (m)

L 2 :

Axial distance of last nozzle to the interface (m)

L :

Length of the vortex chamber (m)

Nu :

Nusslet number, qwDh /λ (Tw -Ti)

Nu a :

Averaged Nusselt number

Nu :

Nusselt number for non-swirling flow in a smooth pipe

ΔP:

Difference between inlet and local pressure (Pa)

P si :

Static pressure of the inlet (Pa)

P so :

Static pressure of the outlet (Pa)

q w :

Wall heat flux (W/m2)

Re :

Reynolds number

T i :

Inlet temperature (K)

T w :

Target wall temperature (K)

U :

Mean axial velocity (m/s)

V i :

Area-averaged velocity of the inlet (m/s

ρ :

Fluid density (kg/m3)

Λ :

Fluid thermal conductivity (W/(m·K))

μ :

Average dynamic viscosity coefficient (kg/(m·s)

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Fan, X., Xue, Y. Numerical investigation of nozzle geometry influence on the vortex cooling in an actual gas turbine blade leading edge cooling system. Heat Mass Transfer 58, 575–586 (2022). https://doi.org/10.1007/s00231-021-03131-9

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