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Handbook of Turbomachinery Second Edition Revised - Ventech!

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tend to be large, due to the necessity <strong>of</strong> modeling in three dimensions not<br />

only multiple blade rows but also multiple blade passages, in order to<br />

achieve a periodic segment <strong>of</strong> the annulus. Such computational requirements<br />

can rapidly exceed the time constraints and computer resources <strong>of</strong><br />

most component design efforts at the present time.<br />

One approach to avoid the massive amounts <strong>of</strong> calculation time<br />

required for an unsteady 3D blade-row interaction analysis is to perform a<br />

steady-flow solution for each individual blade row, and communicate<br />

circumferentially averaged flow conditions between adjacent blade rows via<br />

a mixing plane. Because the flow field at each mixing plane is essentially<br />

time-averaged, nonperiodic circumferential conditions that result from<br />

dissimilar blade counts are not an issue. Therefore, only one passage needs<br />

to be analyzed for each blade row. As a result, the problem size and<br />

calculation time are considerably reduced, compared to an unsteady bladerow<br />

interaction analysis. The mixing plane approach has been taken by<br />

Dawes [62], with his multistage program, and has also been applied to the<br />

method <strong>of</strong> Hah and Wennerstrom [63].<br />

Adamczyk [64] has developed an alternative approach for multiple<br />

blade-row analyses, which utilizes an ‘‘average-passage’’ model. The<br />

governing equations in this model provide a time-averaged 3D representation<br />

<strong>of</strong> the flow through a typical passage <strong>of</strong> each blade row. Individual<br />

solutions are performed for each blade row, with the effects <strong>of</strong> adjacent rows<br />

being modeled by averaged blockage and body forces. A correlation model<br />

is used to represent the interaction between blade rows. The computational<br />

cost <strong>of</strong> the average-passage model is intermediate between the mixing plane<br />

model and the unsteady blade-row interaction analysis. However, the<br />

average-passage simulation becomes more complex and costly as the<br />

number <strong>of</strong> blade rows increases.<br />

The decision to utilize a full unsteady analysis technique depends<br />

largely on what type <strong>of</strong> information is desired. If only time-averaged flow<br />

properties are <strong>of</strong> interest, then a steady, isolated blade-row analysis or a<br />

simplified blade-row interaction model should suffice, with a considerable<br />

savings in computational effort. However, in other cases, the ability to<br />

resolve the time-unsteady nature <strong>of</strong> the flow is essential, to model such<br />

effects as vortex shedding, wake passage, or blade-row interaction. Then a<br />

full unsteady analysis is required.<br />

Numerical Solution Techniques<br />

The subject <strong>of</strong> numerical solution techniques is too extensive to be covered<br />

in any detail in this chapter. Only a cursory discussion <strong>of</strong> methods<br />

appropriate to the solution <strong>of</strong> the time-dependent Reynolds-averaged<br />

Copyright © 2003 Marcel Dekker, Inc.

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