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Handbook of Turbomachinery Second Edition Revised - Ventech!

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Figure 14 Time-space static pressure contours on suction surface at 90% span<br />

under different inlet distortion wavelengths.<br />

while for the case with a long length scale [Fig. 14(b)] the moving shock<br />

covers nearly 50% chord. Clearly, this long wavelength case with a large<br />

shock oscillation is strongly nonlinear.<br />

Given the importance <strong>of</strong> circumferential length scales, one should be<br />

cautious about the practice <strong>of</strong> ‘‘slightly’’ changing blade counts to obtain a<br />

much reduced multipassage computational domain—a drastic change in the<br />

corresponding circumferential wavelength by doing so may result in a very<br />

different unsteady response!<br />

Phasing <strong>of</strong> Unsteady Disturbances<br />

It must be kept in mind that influences <strong>of</strong> an unsteady disturbance depend<br />

on its phase angle, not just the amplitude. The most obvious example is the<br />

use <strong>of</strong> ‘‘antisound’’ where an acoustical noise disturbance can be completely<br />

cancelled by artificially introducing an acoustical disturbance with the same<br />

amplitude but a 1808 phase shift.<br />

Phasing Between Wake and Potential Disturbances<br />

In the context <strong>of</strong> blade forced responses, there is a scope <strong>of</strong> utilizing the<br />

phase difference between wake and potential disturbances to produce<br />

positive results. For example, a higher unsteady loading might not<br />

Copyright © 2003 Marcel Dekker, Inc.

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