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Handbook of Turbomachinery Second Edition Revised - Ventech!

Handbook of Turbomachinery Second Edition Revised - Ventech!

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Figure 16 Time resolved heat transfer measurements and predictions at 08<br />

incidence, Abhari et al. [41].<br />

blade. Variations in magnitude <strong>of</strong> about a factor <strong>of</strong> up to 8 occur at each<br />

measurement point, but location on the blade surface is by far the most<br />

important determiner <strong>of</strong> heat-flux magnitude.<br />

The results <strong>of</strong> the prediction are also given. The code is the 2D thinlayer<br />

Navier–Stokes code, called UNSFLO, developed by Giles and<br />

described in [42]. The code generally does very well, at least in a qualitative<br />

sense, at predicting the variation <strong>of</strong> heat flux with rotor position. Heat-flux<br />

magnitude is sometimes greater than observed and sometimes lower. In<br />

comparing the differences between incidence angles, it is the stagnation<br />

point and the suction side near the leading edge that seem to differ most.<br />

This is probably due the fluctuating state <strong>of</strong> the boundary layer as the wakes<br />

and shocks move over the leading edge and into the rotor passage. Much<br />

more concerning the detailed flow structure is given in [42].<br />

Aerodynamic performance measurements made in short-duration<br />

facilities have been relatively few to date due mostly to concerns about<br />

accuracy. One can argue, however, that with proper care acceptable<br />

aerodynamic results are possible. Figure 17 shows results from aturbine<br />

vane cascade test in the AFRL TRF (Joe et al. [45]), which measured<br />

loading and loss, velocity traverses, and uncooled vane surface heat flux.<br />

Copyright © 2003 Marcel Dekker, Inc.

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