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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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TABLE 9.4. Calculated values <strong>of</strong> flow angles for<br />

Example 9.4<br />

Parameter Ratio r/rt<br />

0.4 0.7 1.0<br />

c q 2 m/s 9.955 5.687 3.982<br />

tan a 2 0.835 0.4772 0.334<br />

a 2 (deg) 39.86 25.51 18.47<br />

U/c x2 1.019 1.7832 2.547<br />

b 2 (deg) 10.43 52.56 65.69<br />

b 3 (deg) 45.54 60.72 68.57<br />

Hydraulic Turbines 313<br />

where the blade tip speed is U 2 =WD 2/2 = (200 ¥ p/30) ¥ 2.9/2 = 30.37m/s<br />

Values a 2, b 2 <strong>and</strong> b 3 shown in Table 9.4 have been derived from the following<br />

relations:<br />

Finally, Figure 9.18 illustrates the variation <strong>of</strong> the flow angles, from which the large<br />

amount <strong>of</strong> blade twist mentioned earlier can be inferred.<br />

Effect <strong>of</strong> size on turbomachine efficiency<br />

Despite careful attention to detail at the design stage <strong>and</strong> during manufacture it is a<br />

fact that small turbomachines always have lower efficiencies than larger geometrically<br />

similar machines. The primary reason for this is that it is not possible to establish perfect<br />

dynamical similarity between turbomachines <strong>of</strong> different size. In order to obtain this<br />

condition, each <strong>of</strong> the the dimensionless terms in eqn. (1.2) would need to be the same<br />

for all sizes <strong>of</strong> a machine.<br />

To illustrate this consider a family <strong>of</strong> turbomachines where the loading term, y =<br />

gH/N 2 D 2 is the same <strong>and</strong> the Reynolds number, Re = ND 2 /n is the same for every size<br />

<strong>of</strong> machine, then

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