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Handbook of Turbomachinery Second Edition Revised - Ventech!

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tangentially to the inner wall, behaves initially as quasi-impingement and<br />

becomes unstable due to interaction with the concave surface <strong>of</strong> a circular<br />

channel. The swirl motion results in a longer path for coolant air to travel<br />

for a given axial length. Highly turbulent flow near the surface leads to a<br />

thin boundary layer. Additional cooling benefits can be obtained due to<br />

centrifugal forces, which push the cool high-density air toward the hot<br />

surface. The Go¨rtler vortices are known to significantly enhance heat<br />

transfer by its downwash and upwash vortical motion near the wall and by<br />

continuous interaction and intermingling with each other.<br />

A comparison <strong>of</strong> the three different swirl cooling configurations versus<br />

impingement cooling with and without cross flow and versus smooth and<br />

trip-strip augmented channel surface is presented in Fig. 22. For the purpose<br />

<strong>of</strong> this comparison, the Nusselt number based on hydraulic diameter was<br />

calculated and averaged over +60 angle from the leading edge. Reynolds<br />

numbers were calculated based on the assumptions that all <strong>of</strong> the flow went<br />

through the cross-sectional area <strong>of</strong> the leading-edge chamber. For<br />

impingement cooling, Chupp and Helm’s correlation (1968) was used for<br />

a given geometry: D=dn ¼ 4, and xn=dn ¼ 3. Kercher and Tabak<strong>of</strong>f’s data<br />

(1970) were used for cross-flow effects on the impingement cooling. The heat<br />

transfer in a channel with normal trip-strips was obtained from the<br />

correlation <strong>of</strong> Webb et al. (1971) [88]. It can be seen from Fig. 21 that the<br />

Figure 22 Comparison <strong>of</strong> internal blade-cooling techniques.<br />

Copyright © 2003 Marcel Dekker, Inc.

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