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Handbook of Turbomachinery Second Edition Revised - Ventech!

Handbook of Turbomachinery Second Edition Revised - Ventech!

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U ¼ rotor tangential velocity.<br />

By inspection, we can see that Eq. (14) relates the square <strong>of</strong> the rotor speed<br />

(and thus, the rotor’s specific kinetic energy) to a change in fluid energy. In<br />

this way, C can be thought <strong>of</strong> as an energy ratio—that is, the fraction <strong>of</strong><br />

rotor kinetic energy that is transferred as energy to the pumped fluid.<br />

As with numerous other design parameters, care and consistency in<br />

usage is <strong>of</strong> great importance. For example, we could refer to the head<br />

coefficient <strong>of</strong> a rotor alone, or <strong>of</strong> an entire pump stage. While these values<br />

would probably be not too different, energy losses between the outlet <strong>of</strong> a<br />

rotor and the outlet <strong>of</strong> a stage would result in C pump being less than C<br />

rotor. Also, when applied to a multistage pumping machine, specificity is<br />

required to understand whether C is specified for an entire pump or just one<br />

(or possibly more than one) stage.<br />

ROCKET PROPULSION SYSTEMS—CENTRIFUGAL PUMPS<br />

Centrifugal pumps (both single and multistage) dominate the design <strong>of</strong><br />

propellant pumping elements for liquid rocket engine systems. There are<br />

several reasons for this.<br />

First, centrifugal machines are normally fairly simple (both hydrodynamically<br />

and otherwise) and rugged. Because <strong>of</strong> the change in radius<br />

through which the pumped fluid is processed, centrifugal stages possess<br />

relatively high head coefficients. This normally results in only a single pump<br />

stage being required for most cases (with the exception <strong>of</strong> very high head<br />

liquid hydrogen pumps).<br />

The relative hydrodynamic simplicity <strong>of</strong> centrifugal stages results in a<br />

decreased requirement for diffusion within the pump. This makes the<br />

centrifugal machine relatively forgiving <strong>of</strong> changes in the operating point at<br />

which it is forced to function. This consideration is particularly important<br />

for an engine system that must operate over a range <strong>of</strong> thrust levels. Since<br />

the H–Q characteristic for the rocket engine system and that for the<br />

centrifugal pump are not the same shape (see Fig. 19), the pump is forced to<br />

operate ‘‘<strong>of</strong>f-design’’ at all operating points except the ‘‘design point.’’<br />

Stability <strong>of</strong> the pump’s operation over this range (and <strong>of</strong>ten a somewhat<br />

larger range) is mandatory for these variable thrust engine systems.<br />

Since the centrifugal pump is capable <strong>of</strong> delivering relatively high head<br />

per stage, these machines generally result in a minimum length <strong>of</strong> the<br />

turbopump rotor assembly. This is important, since long bearing spans<br />

<strong>of</strong>ten contribute to rotor dynamic difficulties, especially at high operating<br />

speeds.<br />

Copyright © 2003 Marcel Dekker, Inc.

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