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Mechanics of Fluids

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660 Fluid machines<br />

in the impeller if 50% <strong>of</strong> the velocity head at outlet from the<br />

impeller is recovered as static head in the volute.<br />

13.14 The impeller <strong>of</strong> a centrifugal fan has an inner radius <strong>of</strong> 250 mm<br />

and width <strong>of</strong> 187.5 mm; the values at exit are 375 mm and<br />

125 mm respectively. There is no whirl at inlet, and at outlet<br />

the blades are backward-facing at 70 ◦ to the tangent. In<br />

the impeller there is a loss by friction <strong>of</strong> 0.4 times the kinetic<br />

head corresponding to the relative outlet velocity, and in the<br />

volute there is a gain equivalent to 0.5 times the kinetic head<br />

corresponding to the absolute velocity at exit from the runner.<br />

The discharge <strong>of</strong> air is 5.7 m 3 · s −1 when the rotational<br />

speed is 84.8 rad · s −1 (13.5 rev/s). Neglecting the thickness <strong>of</strong><br />

the blades and whirl slip, determine the head across the fan<br />

and the power required to drive it if the density <strong>of</strong> the air is<br />

sensibly constant at 1.25 kg · m −3 throughout and mechanical<br />

losses account for 220 W.<br />

13.15 A centrifugal fan, for which a number <strong>of</strong> interchangeable<br />

impellers are available, is to supply air at 4.5 m 3 · s −1 to<br />

a ventilating duct at a head <strong>of</strong> 100 mm water gauge. For<br />

all the impellers the outer diameter is 500 mm, the breadth<br />

180 mm and the blade thickness negligible. The fan runs at<br />

188.5 rad · s −1 (30 rev/s). Assuming that the conversion <strong>of</strong><br />

velocity head to pressure head in the volute is counterbalanced<br />

by the friction losses there and in the impeller, that<br />

there is no whirl at inlet and that the air density is constant at<br />

1.23 kg · m −3 , determine the most suitable outlet angle <strong>of</strong> the<br />

blades. (Neglect whirl slip.)<br />

13.16 A centrifugal pump which runs at 104.3 rad · s −1 (16.6 rev/s) is<br />

mounted so that its centre is 2.4 m above the water level in the<br />

suction sump. It delivers water to a point 19 m above its centre.<br />

For a flow rate <strong>of</strong> Q (m 3 · s −1 ) the friction loss in the suction<br />

pipe is 68Q 2 m and that in the delivery pipe is 650Q 2 m. The<br />

impeller <strong>of</strong> the pump is 350 mm diameter and the width <strong>of</strong><br />

the blade passages at outlet is 18 mm. The blades themselves<br />

occupy 5% <strong>of</strong> the circumference and are backward-facing<br />

at 35 ◦ to the tangent. At inlet the flow is radial and the<br />

radial component <strong>of</strong> velocity remains unchanged through the<br />

impeller. Assuming that 50% <strong>of</strong> the velocity head <strong>of</strong> the water<br />

leaving the impeller is converted to pressure head in the volute,<br />

and that friction and other losses in the pump, the velocity<br />

heads in the suction and delivery pipes and whirl slip are<br />

all negligible, calculate the rate <strong>of</strong> flow and the manometric<br />

efficiency <strong>of</strong> the pump.<br />

13.17 A single-stage centrifugal pump is to be used to pump water<br />

through a vertical distance <strong>of</strong> 30 m at the rate <strong>of</strong> 45 L · s −1 .<br />

Suction and delivery pipes will have a combined length <strong>of</strong> 36 m<br />

and a friction factor f <strong>of</strong> 0.006. Both will be 150 mm diameter.

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