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Handbook of Turbomachinery Second Edition Revised - Ventech!

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Fig. 25. The nature <strong>of</strong> the flow in this cavity is somewhat reminiscent <strong>of</strong> the<br />

distribution over a turbine disk, and load predictions are subject to<br />

essentially the same uncertainties as the turbine disk problem. Again, Refs. 9<br />

and 10 can provide us with some useful insight.<br />

The fluid momentum thrust associated with inducers is due mainly to<br />

their tapered geometry. Contemporary high-performance inducers generally<br />

have tapered hubs, and they may or may not have tapered tips. This results<br />

in an increase in the fluid axial momentum across the inducer. This taper is<br />

shown clearly in Fig. 25.<br />

Centrifugal pumping elements are easily the most popular pumping<br />

elements in use in rocket turbomachinery. As such, their axial thrust<br />

characteristics are <strong>of</strong> great interest. Figure 26 shows a cross section <strong>of</strong> a<br />

‘‘generic’’ centrifugal pumping element and some <strong>of</strong> the forces acting on it.<br />

As in the case <strong>of</strong> the elements discussed previously, axial forces are<br />

generated due to fluid axial momentum changes as well as pressure forces.<br />

Referring to the figure, the pressure force F 1 associated with the impeller<br />

inlet area and pressure is readily calculable. The force F2 is associated with<br />

the change in pumped fluid axial momentum. Using the conservation <strong>of</strong><br />

momentum, this is also calculable, although great care needs to be exercised<br />

with regard to the nature <strong>of</strong> the fluid exit velocity. Although a radial-flow<br />

impeller is shown in the figure, this is not the case with many machines. A<br />

series <strong>of</strong> higher specific speed impellers (known as Francis impellers) is<br />

commonly used in rocket turbomachines. These impellers expel fluid with a<br />

velocity that contains an axial component, and this must be accounted for if<br />

axial thrust computations are to be done accurately. The forces shown as F3<br />

and F4 are pressure forces exerted on the front and rear shrouds <strong>of</strong> the<br />

impeller, respectively. These pressure forces vary with radius and are due to<br />

the recirculating flow that exists between the impeller discharge and its inlet<br />

Figure 26 Centrifugal pump stage axial thrust components: F 1, impeller inlet<br />

pressure force; F2, impeller momentum thrust force; F3, impeller leakage pressure<br />

force; F4, impeller rear face (hub) pressure force.<br />

Copyright © 2003 Marcel Dekker, Inc.

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