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

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252 <strong>Centrifugal</strong> <strong>Pumps</strong>: <strong>Design</strong> <strong>and</strong> <strong>Application</strong><br />

the pr<strong>ed</strong>ict<strong>ed</strong> performance by analysis. A modern computer program<br />

may be us<strong>ed</strong> to perform the calculations, print out the results, <strong>and</strong> also<br />

plot the performance curve.<br />

The pr<strong>ed</strong>iction proc<strong>ed</strong>ure generally consists of accounting for the various<br />

components that compose the total head characteristics. These are<br />

friction losses, absorb<strong>ed</strong> head, shock loss, <strong>and</strong> outlet loss. Power losses<br />

due to internal leakage, disc friction, <strong>and</strong> mechanical losses are also calculat<strong>ed</strong><br />

or estimat<strong>ed</strong> as appropriate. The calculations are made using the<br />

requir<strong>ed</strong> turbine spe<strong>ed</strong>, flow capacities, viscosity, specific gravity of the<br />

fluid, <strong>and</strong> various combinations of mechanical data requir<strong>ed</strong> for certain<br />

multi-stage turbines. There are many publications that cover basic theory<br />

<strong>and</strong> design of pumps that show how to calculate the head <strong>and</strong> loss components<br />

for pumps. These also apply to hydraulic turbines.<br />

Friction losses. Certain components of the total dynamic head are attribut<strong>ed</strong><br />

to friction losses. These are due to flow through the cases, volute<br />

nozzles, diffusers, guide vanes, <strong>and</strong> runners (impellers) as appropriate,<br />

These losses may be simply calculat<strong>ed</strong> as the resistance to the incompressible<br />

flow of fluid in a pipe, using appropriate friction factors, length to<br />

diameter (or hydraulic radius) ratios, <strong>and</strong> the velocity head.<br />

Absorb<strong>ed</strong> head. The absorb<strong>ed</strong> head is deriv<strong>ed</strong> from the well-known<br />

Euler's equations <strong>and</strong> velocity triangles, which have general validity for<br />

all conditions of flow through turbomachines. Refer to Figure 14-4 for<br />

illustration. In practice, the true velocities of flow <strong>and</strong> direction are<br />

never known. The idealiz<strong>ed</strong> velocity triangles of the Euler head equation<br />

assume perfect guidance of the flow by the vanes. It is known that there<br />

is a deviation of the fluid from the vane direction, which is the phenomenon<br />

call<strong>ed</strong> "slip." This is a consequence of the nonuniform velocity distribution<br />

across the runner channels, boundary-layer accumulation, <strong>and</strong><br />

any separation.<br />

Actual pr<strong>ed</strong>iction of "slip" cannot be pr<strong>ed</strong>etermin<strong>ed</strong> in a practical<br />

manner. However, it has been found that "slip" factors us<strong>ed</strong> for pump<br />

design appli<strong>ed</strong> to the turbine outlet vectors produce good results. The absolute<br />

velocity at the runner inlet (Cj) is the average velocity of the liquid<br />

at the nozzles with a free vortex correction appli<strong>ed</strong> to account for the distance<br />

from the nozzles to the runner. The nozzles are the highest velocity<br />

throat areas of the volute cases, diffusers, or guide vanes as appropriate<br />

for the turbine construction.<br />

Shock loss. The shock loss component of the total dynamic head is calculat<strong>ed</strong><br />

as the velocity head (V s 2 /2g) due to the mismatch of the absolute

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