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Large-eddy Simulation of Realistic Gas Turbine Combustors

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300 (a)<br />

200<br />

(b)<br />

Axial Velocity<br />

200<br />

100<br />

0<br />

Swirl Velocity<br />

100<br />

0<br />

-100<br />

-100<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

-200<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

Axial Velocity<br />

200<br />

150<br />

100<br />

50<br />

0<br />

-50<br />

(c)<br />

Swirl Velocity<br />

150<br />

100<br />

50<br />

0<br />

-50<br />

-100<br />

(d)<br />

-100<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

-150<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

200<br />

(e)<br />

100<br />

(f)<br />

Axial Velocity<br />

100<br />

0<br />

Swirl Velocity<br />

50<br />

0<br />

-50<br />

-100<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

Normalized Radius<br />

-100<br />

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2<br />

Normalized Radius<br />

Figure 8: Radial variation <strong>of</strong> normalized mean axial and swirl velocities at different axial locations<br />

for the PW injector patternation study: ◦ experimental data [25], LES, Unsteady RANS<br />

using k − ɛ model: (a-b) x = 0.4, (c-d) x = 1.1, (e-f) x = 2.1. Here x is the normalized distance<br />

from the injector wall.<br />

34

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