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Handbook of Turbomachinery Second Edition Revised - Ventech!

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System Disruptions Leading to Rotor Torsional Modes. Rotor torsional<br />

vibrations can be excited by electrical faults in the distribution system. These<br />

torsional vibrations can lead to considerable damage to the rotor and<br />

blading and have led to a number <strong>of</strong> blade failures in the power industry<br />

[55]. The turbine generator system may respond to subsynchronous,<br />

synchronous, or supersynchronous (typically two times the running speed,<br />

e.g., 120 Hz for 60-Hz turbines) frequencies.<br />

Design <strong>of</strong> pre-1975 machines typically evaluated the potential for<br />

synchronous vibrations, but were not designed for frequency resonances<br />

equal to two times the running speed. These resonances occur as a result <strong>of</strong><br />

load imbalance on the three phases which can induce secondary currents in<br />

the generator stator. These stator currents, termed ‘‘negative sequence<br />

currents,’’ cause an alternating torque to act on the rotor system at twice the<br />

transmission grid frequency <strong>of</strong> 60 Hz. Sources <strong>of</strong> such load imbalance can<br />

include: cut<strong>of</strong>f <strong>of</strong> load, line accidents, subsynchronous resonance, or a short<br />

in the generator terminals [73, 74].<br />

Torsional modes near this frequency tend to be highly coupled to<br />

disk–blade modes and, as a result, considerable high cycle fatigue damage<br />

can be imparted to LP blades, particularly in the last stages, from the<br />

phenomenon illustrated schematically in Fig. 42. Failures caused by this<br />

mechanism have been reported in fossil units and in nuclear units.<br />

A number <strong>of</strong> researchers have reported on the analysis <strong>of</strong> disk–blade<br />

interactions, specifically related to avoiding unwanted resonances (see, for<br />

example, Refs. [55–63]). The aims <strong>of</strong> such analyses are to evaluate blade and<br />

disk dynamics and to avoid resonances with the electrical grid frequency.<br />

Two examples illustrate the typical methodology.<br />

Higuchi and Tsuda performed a torsional vibration analysis <strong>of</strong> the LP<br />

turbine in a 1,160-MW nuclear unit; <strong>of</strong> particular concern were frequencies<br />

near 120 Hz. They found as many as 45 torsional natural modes in the<br />

frequency range below 180 Hz. The natural modes included fundamental<br />

modes, higher modes <strong>of</strong> the shaft, and blade–shaft interactions. Torsional<br />

modes above 70 Hz were mostly caused by coupled effects between the<br />

blade, shaft, and disk. Field tests measured the blade induced vibrations<br />

caused by short circuits induced at the generator terminals and concluded<br />

that, in this case, the blades <strong>of</strong> the L-0 row were tuned well away from<br />

120 Hz.<br />

Reid provided a detailed case study that evaluated coupled blade–<br />

rotor torsional vibration in anticipation <strong>of</strong> a major low-pressure blade<br />

retr<strong>of</strong>it. That analysis analyzed the natural frequencies and response stresses<br />

for a system that included a combined HP, IP and two LP turbines along<br />

with a generator and exciter. Bladed disks were modeled as branch elements.<br />

The model developed was confirmed using impact or ‘‘bump’’ testing on the<br />

Copyright © 2003 Marcel Dekker, Inc.

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