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Handbook of Turbomachinery Second Edition Revised - Ventech!

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Figure 15k H–Q characteristics for several typical pumps.<br />

could fall along the curve labeled ‘‘shallow depth <strong>of</strong> stall’’ in Fig. 15(k). The<br />

principle here is simply that the more diffuser rows continue to operate, the<br />

shallower is the depth <strong>of</strong> stall. On the other hand, if a diffuser in one <strong>of</strong> the<br />

‘‘early’’ stages <strong>of</strong> the pump stalls, the velocity diagrams in all subsequent<br />

stages are likely to be upset, resulting in a near total collapse <strong>of</strong> their<br />

developed head. The further toward the pump inlet the stall propagates, the<br />

steeper is the depth <strong>of</strong> stall.<br />

The propensity <strong>of</strong> multistage axial-flow pumps to perform in the<br />

manner described above has discouraged their application in modern liquid<br />

rocket engine systems. It should also be noted that attempts at ‘‘aggressive’’<br />

packaging for weight savings (i.e., fewer pump stages, more highly loaded<br />

stages, etc.) will only aggravate this tendency. It is a fact that axial-flow<br />

pumps designed with an effort toward weight conservation have been unable<br />

to support significant thrust-level changes <strong>of</strong> the engine systems and, in one<br />

instance, have been unable to support the engine system starting transient.<br />

In this last case, elaborate prestart procedures and special control system<br />

considerations were necessary to ensure satisfactory engine starts.<br />

Inducers<br />

The continued tendency to optimize launch vehicle design for minimum<br />

inert structural weight is well known. Since the propellant tanks <strong>of</strong> a large<br />

liquid propellant launch vehicle are typically the largest pieces <strong>of</strong> vehicle<br />

Copyright © 2003 Marcel Dekker, Inc.

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