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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

Vapour pressure as head <strong>of</strong> water, m<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

According to eqn. (1.12b), when W SS exceeds 4.0 (rad) then cavitation can occur, giving<br />

further confirmation <strong>of</strong> the above conclusion.<br />

Connection between Thoma’s coefficient, suction specific speed <strong>and</strong><br />

specific speed<br />

The definitions <strong>of</strong> suction specific speed <strong>and</strong> specific speed are<br />

Combining <strong>and</strong> using eqn. (9.24), we get<br />

0 10 20 30 40<br />

Temperature, ∞C<br />

FIG. 9.20. Vapour pressure <strong>of</strong> water as head (m) vs temperature.<br />

(9.26)<br />

Exercise. Verify the value <strong>of</strong> Thoma’s coefficient in the earlier example using<br />

the values <strong>of</strong> power specific speed, efficiency <strong>and</strong> suction specific speed given or<br />

derived.<br />

We use as data WSS = 7.613, WSP = 0.8 <strong>and</strong> hH = 0.896 so that, from eqn. (1.9c),

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