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Centrifugal Pumps Design and Application 2nd ed - Val S. Lobanoff, Robert R. Ross (Butterworth-Heinemann, 1992)

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Vibration <strong>and</strong> Noise in <strong>Pumps</strong> 443<br />

A thorough lateral critical spe<strong>ed</strong> analysis is essential for developing a<br />

reliable, trouble-free pump system. The design audit [18] should include<br />

the following calculations:<br />

• Critical spe<strong>ed</strong> map<br />

• Undamp<strong>ed</strong> natural frequencies <strong>and</strong> mode shapes<br />

• Bearing stiffness <strong>and</strong> damping properties<br />

• Seal stiffness <strong>and</strong> damping properties<br />

• Rotor response to unbalance<br />

• P<strong>ed</strong>estal <strong>and</strong> foundation effects on response<br />

• Rotor stability<br />

The first step in performing a lateral critical spe<strong>ed</strong> analysis is to model<br />

the shaft with sufficient detail <strong>and</strong> number of masses to accurately simulate<br />

the rotor responses through its spe<strong>ed</strong> range. An accurate shaft drawing<br />

giving the dimensions, weights, <strong>and</strong> centers of gravity of all add<strong>ed</strong><br />

masses is ne<strong>ed</strong><strong>ed</strong> to develop the model. Generally, each significant shaft<br />

diameter change is represent<strong>ed</strong> by one or more stations. A station is generally<br />

locat<strong>ed</strong> at each add<strong>ed</strong> mass or inertia, at each bearing <strong>and</strong> seal location,<br />

<strong>and</strong> at each potential unbalance location. A typical rotor shaft<br />

drawing <strong>and</strong> the computer model is given in Figure 18-9.<br />

Rotating elements such as impellers are model<strong>ed</strong> as add<strong>ed</strong> masses <strong>and</strong><br />

inertias at the appropriate locations on the shaft. The polar <strong>and</strong> transverse<br />

mass moments of inertia are includ<strong>ed</strong> in the analyses to simulate the<br />

gyroscopic effects on the rotor. The gyroscopic effects are particularly<br />

significant on overhung rotors where the impeller produces a restoring<br />

moment when whirling in a deflect<strong>ed</strong> position.<br />

Couplings are simulat<strong>ed</strong> as concentrat<strong>ed</strong> add<strong>ed</strong> weights <strong>and</strong> inertias.<br />

Normally half the coupling weight is plac<strong>ed</strong> at the center of gravity of the<br />

half coupling. When necessary, the entire train, including the driver <strong>and</strong><br />

driven equipment, can be model<strong>ed</strong> by utilizing programs that can simulate<br />

the shear loading <strong>and</strong> moment transfer across the coupling. Once the<br />

shaft model is complet<strong>ed</strong>, the critical spe<strong>ed</strong> map can be calculat<strong>ed</strong>,<br />

Critical Spe<strong>ed</strong> Map. The critical spe<strong>ed</strong> map is a logarithmic plot of the<br />

undamp<strong>ed</strong> lateral critical spe<strong>ed</strong>s versus the combin<strong>ed</strong> support stiffness,<br />

consisting of the bearing <strong>and</strong> support structure as springs in series. The<br />

critical spe<strong>ed</strong> map provides the information ne<strong>ed</strong><strong>ed</strong> to underst<strong>and</strong> the basic<br />

response behavior of rotors; therefore, it is important to underst<strong>and</strong><br />

how the map is develop<strong>ed</strong> [25].<br />

For large values of support stiffness, the rotor critical spe<strong>ed</strong>s are call<strong>ed</strong><br />

the rigid bearing critical spe<strong>ed</strong>s. If the bearing stiffness is infinity, the<br />

vibrations are zero at the bearings, <strong>and</strong> the first natural frequency for

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