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Handbook of Turbomachinery Second Edition Revised - Ventech!

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in the section on blade cooling that follows, where application <strong>of</strong> film<br />

cooling is <strong>of</strong>ten somewhat limited compared to nozzles.<br />

Film-cooling application for turbine airfoils is very common in<br />

advanced gas turbines. For this reason the following section considers most<br />

<strong>of</strong> the factors that influence film cooling. A comprehensive early guide to the<br />

methodology <strong>of</strong> film cooling was given by Goldstein (1971) [42]. However,<br />

these generic early data have very limited application for the modern airfoil<br />

shapes and realistic main-stream velocity distribution. The most recent<br />

bibliography <strong>of</strong> the film cooling can be found in [43, 44].<br />

With film cooling the heat flux q 00<br />

f is given by the following relation:<br />

q 00<br />

f ¼ hfðTaw TwÞ; the heat-transfer coefficient, hf, is <strong>of</strong>ten assumed to be<br />

that which would exist without film injection, although it may deviate<br />

significantly from this value in the near-hole region. The adiabatic wall<br />

temperature Taw is the temperature assumed at the wall in the absence <strong>of</strong><br />

heat flow (without film cooling, the adiabatic wall temperature for low<br />

Mach number is equal to the main-stream gas temperature), and Tw is the<br />

actual wall temperature. In the presence <strong>of</strong> film cooling, the adiabatic wall<br />

temperature is defined by a dimensionless wall temperature called filmcooling<br />

effectiveness generally designated by Z and defined as<br />

where<br />

Z ¼ðTg TfÞ=ðTg TcÞ<br />

Tg and Tc are the gas stream and coolant exit temperatures,<br />

respectively.<br />

Tf is the film temperature (adiabatic wall temperature resulting from<br />

film injection).<br />

The film temperature is a function <strong>of</strong> distance downstream from the<br />

injection point and must be experimentally determined for a given filmcooling<br />

geometry. Film temperature is generally correlated in terms <strong>of</strong> local<br />

film effectiveness as<br />

Tf ¼ Tg ZðTg TcÞ<br />

There are two main types <strong>of</strong> geometry used in film cooling: slots and<br />

rows <strong>of</strong> discrete holes. However, slots are not <strong>of</strong>ten used in airfoils because<br />

<strong>of</strong> thermal stress and mechanical design considerations. High thermal<br />

stresses are caused by the fact that the airfoil region just upstream <strong>of</strong> a slot is<br />

hot, while just downstream <strong>of</strong> a slot it is cold. Provision <strong>of</strong> slots causes<br />

difficulty in holding the airfoil together at the slot, especially in the presence<br />

<strong>of</strong> the high thermal stresses. Replacing the slot with a row <strong>of</strong> holes tends to<br />

reduce these problems considerably because the metal between the holes<br />

Copyright © 2003 Marcel Dekker, Inc.

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