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Handbook of Turbomachinery Second Edition Revised - Ventech!

Handbook of Turbomachinery Second Edition Revised - Ventech!

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and also increases the critical speeds to those determined by the bearing<br />

support structure. The structural damping (i.e., 5% <strong>of</strong> critical damping) then<br />

determines the magnitude <strong>of</strong> the unbalance response as the rotor decelerates<br />

through its critical speeds.<br />

The large amplitude response and resulting rubs render the system<br />

nonlinear. Most blade-out unbalance response analyses are conducted using<br />

piecewise linear equivalent springs and dampers at the rub locations. The<br />

rub can be modeled as a bilinear spring with zero stiffness until the<br />

deflection equals the clearance between the rotating assembly (i.e., the blade<br />

tips) and ‘‘hard’’ metal. The stiffness after hard contact is based on the<br />

lateral bending and ovalization <strong>of</strong> the casing. The steady-state response at<br />

each spin-speed is determined using an iterative process, continuing until the<br />

assumed response at each rub location matches the predicted response<br />

within a convergence criterion.<br />

Figure 43 illustrates a typical steady-state blade-out response using the<br />

straddle-mounted example with squeeze film dampers presented earlier.<br />

Assuming a 0.10-in. (2.54 mm) cgx <strong>of</strong> the aft disk after a blade failure and no<br />

rubs, the response at the first critical speed resembles that <strong>of</strong> the hardmounted,<br />

in-phase unbalance case shown in Fig. 39a except it is over 60<br />

times greater. Due to the large rotor whirl both <strong>of</strong> the squeeze film dampers<br />

Figure 43 Steady-state blade-out response: straddle-mounted rotor.<br />

Copyright © 2003 Marcel Dekker, Inc.

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