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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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Hydraulic Turbines 317<br />

using Thoma’s coefficient <strong>and</strong> the data shown in Figure 9.19, determine whether<br />

cavitation is likely to occur. Also using the data <strong>of</strong> Wislicenus verify the result.<br />

Solution. From tables <strong>of</strong> fluid properties, e.g. Rogers <strong>and</strong> Mayhew (1995), or using<br />

the data <strong>of</strong> Figure 9.20, the vapour pressure for water corresponding to a temperature<br />

<strong>of</strong> 25°C is 0.03166 bar. From the definition <strong>of</strong> NPSH, eqn. (9.24), we obtain<br />

Thus, Thoma’s coefficient is, s = HS/H E = 8.003/150 = 0.05336.<br />

At the value <strong>of</strong> WSP = 0.8 given as data, the value <strong>of</strong> the critical Thoma coefficient<br />

sc corresponding to this is 0.09 from Figure 9.19. From the fact that s < sc, then the<br />

turbine will cavitate.<br />

From the definition <strong>of</strong> the suction specific speed<br />

Cavitation coefficient, s<br />

4.0<br />

2.0<br />

1.0<br />

0.4<br />

0.2<br />

0.1<br />

0.04<br />

No cavitation<br />

region<br />

Severe<br />

cavitation<br />

region<br />

Francis turbinesKaplan turbines<br />

0.02<br />

0.1 0.2 0.4 0.6 1.0 2.0 4.0 6 8 10<br />

Power specific speed, Wsp (rad)<br />

FIG. 9.19. Variation <strong>of</strong> critical cavitation coefficient with non-dimensional specific<br />

speed for Francis <strong>and</strong> Kaplan turbines (adapted from Moody <strong>and</strong> Zowski 1969).

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