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Handbook of Turbomachinery Second Edition Revised - Ventech!

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component. Use <strong>of</strong> a hot cascade for steady-state experiments or shortduration<br />

facilities for transient experiments becomes a necessity for<br />

obtaining reliable data and validation <strong>of</strong> the airfoil cooling systems.<br />

Realistically simulated steady-state hot cascade experiments using actual<br />

engine hardware with proper external/internal cooling arrangements can be<br />

extremely beneficial for turbine airfoil local temperature prediction in the<br />

early stage <strong>of</strong> turbine development. A few <strong>of</strong> the experiments using actual<br />

engine configuration were reported [12–16]. However, heat-transfer experiments<br />

including evaluation and comparison <strong>of</strong> the cooling effectiveness in<br />

both engine and hot cascade environments are rarely discussed in the open<br />

literature.<br />

The solutions <strong>of</strong> the Navier–Stokes and energy equations for<br />

compressible flow depend on a number <strong>of</strong> dimensionless groups. These<br />

equations suggest that the similarity <strong>of</strong> fluid streamlines and the isotherms in<br />

forced convection heat transfer can be enforced by using the same<br />

magnitudes <strong>of</strong> these nondimensional groups for both the actual phenomenon<br />

and the simulation experiment. When the momentum and energy<br />

equations are nondimensionalized, the solution strongly depends on four<br />

nondimensional parameters: Re, Gr/Re 2 , 1/(Pr Re), and Ec.<br />

For most <strong>of</strong> the forced convection problems <strong>of</strong> interest to us such as<br />

external heat transfer on a gas turbine blade, buoyancy forces are considered<br />

negligible compared to inertial forces. The Eckert number Ec can be<br />

expressed in terms <strong>of</strong> free-stream Mach number, Ma, wall-to-free-stream<br />

total temperature ratio, and the specific heat ratio: Ec ¼ðg 1ÞMa 2<br />

ðT?=T?0Þ=ð1 Tw=T?0Þ<br />

The static to total temperature ratio can be replaced by using the<br />

isentropic relation, to obtain<br />

Ec ¼ðg 1ÞMa 2 1= 1 þðg 1ÞMa 2 =2 =ð1 Tw=T?0 Þ<br />

STEADY-STATE AND TRANSIENT HEAT-TRANSFER ISSUES<br />

IN THE ENGINE HOT SECTION<br />

Over the past three decades, turbine heat-transfer calculations and<br />

experimental data have been reported in the open literature by numerous<br />

industry, government, and university authors. The detail reported for a<br />

particular calculation generally depends on the competition sensitive nature<br />

<strong>of</strong> the data. Understandably, the company design codes distinguish the<br />

manufacturers, and detail about these codes will be kept proprietary.<br />

Copyright © 2003 Marcel Dekker, Inc.

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