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Handbook of Turbomachinery Second Edition Revised - Ventech!

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(11) for a simple case]:<br />

Where<br />

WA ¼ p XNc<br />

i¼1<br />

½AfAx sinðf fxÞŠ i<br />

ð23Þ<br />

Af is the amplitude <strong>of</strong> the induced aerodynamic force component on<br />

mesh cell i in the direction <strong>of</strong> the vibratory motion.<br />

Ax is the amplitude <strong>of</strong> the vibrating displacement <strong>of</strong> the cell.<br />

f fx is the phase lead <strong>of</strong> the induced aerodynamic force relative to the<br />

displacement for the cell.<br />

Aerodynamic damping can be defined as<br />

DA ¼ WA ð24Þ<br />

The total damping <strong>of</strong> the blade aeroelastic system is<br />

D ¼ DM þ DA<br />

ð25Þ<br />

A conservative prediction can be made by neglecting the mechanical<br />

damping, DM, which is always positive. Aeroelastic stability <strong>of</strong> a blade is<br />

directly indicated by a damping coefficient taking a form <strong>of</strong><br />

CA ¼ WA<br />

A 2 m<br />

ð26Þ<br />

where Am is the maximum vibration amplitude taken in the unsteady<br />

aerodynamic calculation. So, the somehow arbitrary vibrating amplitude<br />

taken in the damping calculation does not matter provided the aerodynamic<br />

response is <strong>of</strong> a linear nature.<br />

Apparently, given natural vibration mode shapes and frequencies, a<br />

blade flutter analysis using the energy method will be solely determined by<br />

unsteady aerodynamic calculations. This is why unsteady aerodynamics<br />

around oscillating blades in a specified mode has attracted so much<br />

attention and effort in flutter analysis and predictions for turbomachinery<br />

blades.<br />

Forced Response Prediction<br />

Forced response is more complex, because it involves two separate<br />

aerodynamic elements, aerodynamic damping and aerodynamic forcing.<br />

The analysis may be most effectively carried out in a Modal space, where<br />

the original structural dynamic equations with N degrees-<strong>of</strong>-freedom are<br />

decoupled into N single-degree-<strong>of</strong>-freedom equations. Each <strong>of</strong> these<br />

Copyright © 2003 Marcel Dekker, Inc.

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