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Handbook of Turbomachinery Second Edition Revised - Ventech!

Handbook of Turbomachinery Second Edition Revised - Ventech!

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Two major practical requirements exist when the turbine rotor–stator<br />

system is developed:<br />

1. Define turbine disc local heat-transfer coefficients for specified<br />

rotational speed, geometry, and disc-cooling configuration.<br />

2. Provide a system that prevents hot gas ingress into the disc<br />

plenum.<br />

Disc heat-transfer prediction based on flow visualization (Pincombe, 1989)<br />

and measured angular velocity <strong>of</strong> the flow core in the plenum between disc<br />

and stator was a traditional method along with complicated direct<br />

measurements <strong>of</strong> the local disc temperatures or heat fluxes.<br />

Some <strong>of</strong> the early flow visualization methods for the air in the plenum<br />

were based on application <strong>of</strong> TiCl4 reacting chemically with the humid air to<br />

produce high-density white smoke. This method <strong>of</strong> flow visualization is<br />

practically obsolete at the present time because <strong>of</strong> product toxicity. It was<br />

noticed (Glezer, 1969) [131] and Phadke and Owen, 1988 [132] that<br />

nonaxisimmetric pressure distribution in the main-stream flow over disc–<br />

stator gap can produce a standing wave pattern <strong>of</strong> ‘‘hot gas’’ ingress into the<br />

plenum even when outward supply <strong>of</strong> ‘‘cooling’’ air flow exceeded disc<br />

pumping flow. (Turbine nozzle vane wakes present a typical example <strong>of</strong><br />

nonaxisimmetric pressure distribution.) This phenomenon has to be<br />

addressed when an actual rotor–stator system is developed.<br />

A very promising experimental technique to study both ‘‘hot gas’’<br />

ingress and local convective heat transfer distribution along turbine disc and<br />

stator, based on application <strong>of</strong> liquid-crystal coating in a thermal transient<br />

test, was described by Metzger et al. [133]. More recent results performed at<br />

ASU for some practical rotor–stator geometries were referred earlier [105].<br />

An additional study <strong>of</strong> effect <strong>of</strong> rotation on the accuracy <strong>of</strong> the liquidcrystal<br />

experiment was performed by Camci et al. [134] who replaced an<br />

acrylic disc with high-strength aluminum disc dressed with a balsa layer that<br />

was required to meet one-dimensional transient response <strong>of</strong> ‘‘semi-infinite<br />

solid.’’ Balsa face surface was painted black and coated with thin liquid<br />

crystal. Coating <strong>of</strong> the disc face and acrylic stator with liquid crystals, which<br />

have significant difference in transitional temperature, allows performing<br />

heat-transfer thermal imagining for both disc and stator during one test.<br />

This approach was used and tested in a full-scale industrial turbine rotor–<br />

stator system rig (Fig. 33). Significant design features required for this rig<br />

included<br />

Full-scale turbine disc with rim seal and preswirler air delivery system<br />

(feeding air into angular disc holes that represent blade-cooling<br />

passages)<br />

Copyright © 2003 Marcel Dekker, Inc.

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