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Handbook of Turbomachinery Second Edition Revised - Ventech!

Handbook of Turbomachinery Second Edition Revised - Ventech!

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in heat transfer as the Reynolds number is increased. The converse is true as<br />

the Mach number is increased. This follows the classical trends for flat-plate<br />

boundary layers, and the only difference in the present case is the effect <strong>of</strong><br />

curvature and pressure gradient which modify the onset and length <strong>of</strong><br />

transition. The effects <strong>of</strong> turbulence are well catalogued by a number <strong>of</strong><br />

authors, for example by Arts et al. [29] and Consigny et al. [30]. Their<br />

studies show (Fig. 12) that as inlet turbulence is increased, the location <strong>of</strong><br />

transition moves upstream and generally leads to an increase in the heat<br />

transfer to the suction side <strong>of</strong> the airfoil.<br />

Curvature<br />

It has been established that the aerodynamics on the pressure side is mainly<br />

two-dimensional. Therefore, the heat transfer on the pressure side is also<br />

mainly two-dimensional and can be predicted, in most cases, using twodimensional<br />

boundary-layer computer programs. It has been observed that<br />

the presence <strong>of</strong> Goertler vortex on concave surfaces [[31] and [32]] (Volino et<br />

al., Dring et al.) can increase the heat transfer to turbine pressure sides<br />

particularly at low inlet turbulence intensity. However, experiments on<br />

actual turbine vanes and blades that exhibit high inlet free-stream<br />

turbulence (Tu > 5%) do not appear to confirm such phenomena. It may<br />

also be that the convex to concave curvature transition near the leading edge<br />

in real engine airfoils (test cascades and engine vanes) eliminates or destroys<br />

the growth <strong>of</strong> the Goertler vortex, which is quite sensitive to curvature<br />

effects and inlet turbulence.<br />

The effect <strong>of</strong> streamwise surface curvature is to stabilize the boundary<br />

layer on a convex surface and to destabilize the boundary layer on a concave<br />

surface. The destabilizing effect <strong>of</strong> centrifugal forces on the concave wall<br />

induces an instability, which results in Goertler vortices with axes in the<br />

same direction as the main-stream flow. It has been shown that the heat<br />

transfer on a concave wall is increased with surface curvature and that for a<br />

convex wall the heat transfer is decreased. Turbulence intensities in the<br />

boundary layer are significantly reduced on a convex wall and enhanced on<br />

a concave wall. The results <strong>of</strong> some studies also suggest that the effect <strong>of</strong><br />

surface curvature is nonlinear, being very strong at small curvature values<br />

but increasing less than proportionately as curvature increases.<br />

Vane suction surfaces are more influenced by secondary flows. It has<br />

been shown that the end-wall boundary layers migrate across the suction<br />

surface <strong>of</strong> the vane. In case <strong>of</strong> a blade, the tip section has a more intensive<br />

secondary flow resulting from the radial pressure gradient (tip to hub) that<br />

tends to push more fluid along the airfoil suction side. The secondary flows<br />

affect the heat transfer close to the tip and hub sections <strong>of</strong> the nozzle.<br />

Copyright © 2003 Marcel Dekker, Inc.

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