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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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312 <strong>Fluid</strong> <strong>Mechanics</strong>, <strong>Thermodynamics</strong> <strong>of</strong> <strong>Turbomachinery</strong><br />

2<br />

3<br />

1<br />

The relations for the flow angles are<br />

r 1<br />

Exit<br />

flow<br />

(9.22a)<br />

(9.22b)<br />

Example 9.4. A small-scale Kaplan turbine has a power output <strong>of</strong> 8MW, an available<br />

head at turbine entry <strong>of</strong> 13.4m <strong>and</strong> a rotational speed <strong>of</strong> 200rev/min. The inlet<br />

guide vanes have a length <strong>of</strong> 1.6m <strong>and</strong> the diameter at the trailing edge surface is<br />

3.1m. The runner diameter is 2.9m <strong>and</strong> the hub–tip ratio is 0.4.<br />

Assuming the hydraulic efficiency is 92% <strong>and</strong> the runner design is “free-vortex”,<br />

determine<br />

(i) the radial <strong>and</strong> tangential components <strong>of</strong> velocity at exit from the guide vanes;<br />

(ii) the component <strong>of</strong> axial velocity at the runner;<br />

(iii) the absolute <strong>and</strong> relative flow angles upstream <strong>and</strong> downstream <strong>of</strong> the runner at<br />

the hub, mid-radius <strong>and</strong> tip.<br />

Solution. As P = hHrgQHE, then the volume flow rate is<br />

As the specific work done is DW = U 2cq2 <strong>and</strong> hH =DW/(gHE), then at the tip<br />

b 2<br />

W 2<br />

U<br />

c 3 = c x<br />

c 2<br />

a 2<br />

Blade motion<br />

FIG. 9.17. Section <strong>of</strong> a Kaplan turbine <strong>and</strong> velocity diagrams at inlet to <strong>and</strong> exit from<br />

the runner.<br />

b 3<br />

U<br />

W 3

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