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Handbook of Turbomachinery Second Edition Revised - Ventech!

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passage domain is required. The method is currently extended to a<br />

multistage environment to analyze rotor–stator and rotor–rotor (stator–<br />

stator) interaction (aperiodic and clocking) effects on both aerothermal and<br />

aeromechanical performances. The whole annulus unsteady flow field is<br />

reconstructed from the single-passage result according to the phase-shifted<br />

periodicity. By introducing the nonrotating spatial harmonics, representing<br />

upstream wakes, the aperiodic disturbances due to different rotor–rotor<br />

blade counts as well as the clocking effects are efficiently included in a<br />

single-passage solution.<br />

Some further comments need to be made on this kind <strong>of</strong> unsteady flow<br />

modeling based on flow decomposition, which is seemingly more complex<br />

(undesirable!) than the straightforward time-domain unsteady CFD<br />

methods. First, the unsteady disturbances we are dealing with are generally<br />

small in magnitudes, though their effects may not be. To ensure small<br />

unsteadiness to be adequately resolved, numerical errors (artificial dissipation<br />

and dispersion) need to be much smaller compared to the physical<br />

signals to give a reasonable ‘‘signal-to-noise’’ ratio. For instance, in the field<br />

<strong>of</strong> computational aeroacoustics, it has been evident that conventional<br />

unsteady CFD algorithms with second-order temporal and spatial<br />

discretizations are unable to adequately extract small but meaningful<br />

physical acoustical disturbances from a background flow. In the context <strong>of</strong><br />

unsteady turbomachinery flows, it won’t be difficult to find situations where<br />

physical unsteady disturbances are easily ‘‘washed <strong>of</strong>f’’ by numerical<br />

dissipations. Since magnitudes <strong>of</strong> numerical errors are normally in<br />

proportion to those <strong>of</strong> flow variables, it would be more accurate to directly<br />

solve the unsteady perturbations. <strong>Second</strong>, by decomposing the timeaveraged<br />

flow and the unsteady part, we can use the same numerical<br />

algorithms and boundary condition treatments for both a time-averaged<br />

flow and a pure steady flow. The past experiences suggest that usefulness <strong>of</strong><br />

comparing different unsteady CFD computations depends measurably on<br />

the consistency <strong>of</strong> the ways these computations are carried out. Hence use <strong>of</strong><br />

the same numerics in both steady and time-averaged calculations should<br />

help to identify and understand true unsteady effects.<br />

Some Comments on Turbulence/Transition Modeling<br />

It has been a standard practice that turbulence models tuned for steady<br />

flows are used quasisteadily for unsteady flows. The uncertainties associated<br />

with this must be recognized. At the same time, it is felt that this should not<br />

always be used as an explanation (or excuse!) for poor agreements between<br />

computational and experimental results. For instance, one may find the<br />

turbulence/transition modeling will strongly affect blade aerodynamic<br />

Copyright © 2003 Marcel Dekker, Inc.

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