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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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Hydraulic Turbines 309<br />

constant. The regulation at part load operation is achieved by varying the angle <strong>of</strong> the<br />

guide vanes. The guide vanes are pivoted <strong>and</strong>, by means <strong>of</strong> a gearing mechanism, the<br />

setting can be adjusted to the optimum angle. However, operation at part load causes<br />

a whirl velocity component to be set up downstream <strong>of</strong> the runner causing a reduction<br />

in efficiency. The strength <strong>of</strong> the vortex can be such that cavitation can occur along the<br />

axis <strong>of</strong> the draft tube (see remarks on cavitation later in this chapter).<br />

Example 9.3. In a vertical-shaft Francis turbine the available head at the inlet flange<br />

<strong>of</strong> the turbine is 150m <strong>and</strong> the vertical distance between the runner <strong>and</strong> the tailrace is<br />

2.0m. The runner tip speed is 35m/s, the meridional velocity <strong>of</strong> the water through the<br />

runner is constant <strong>and</strong> equal to 10.5m/s, the flow leaves the runner without whirl <strong>and</strong><br />

the velocity at exit from the draft tube is 3.5m/s. The hydraulic energy losses estimated<br />

for the turbine are as follows:<br />

Determine<br />

(i) the pressure head (relative to the tailrace) at inlet to <strong>and</strong> at exit from the runner;<br />

(ii) the flow angles at runner inlet <strong>and</strong> at guide vane exit;<br />

(iii) the hydraulic efficiency <strong>of</strong> the turbine.<br />

If the flow discharged by the turbine is 20m 3 /s <strong>and</strong> the power specific speed <strong>of</strong> the<br />

turbine is 0.8 (rad), determine the speed <strong>of</strong> rotation <strong>and</strong> the diameter <strong>of</strong> the runner.<br />

Solution. From eqn. (9.20)<br />

N.B. The head H3 is relative to the tailrace.<br />

i.e. the pressure at runner outlet is below atmospheric pressure, a matter <strong>of</strong> some importance<br />

when we come to consider the subject <strong>of</strong> cavitation later in this chapter. From<br />

eqn. (9.18),<br />

From eqn. (9.18),

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