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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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efficiently converting this energy into pressure energy can be appreciated. The conversion<br />

<strong>of</strong> the kinetic energy to pressure energy is considered in the following section on<br />

diffusers.<br />

The fraction <strong>of</strong> the kinetic energy at impeller exit to the specific work input is<br />

where<br />

Define the total-to-total efficiency <strong>of</strong> the impeller as<br />

where pr is the total-to-total pressure ratio across the impeller, then<br />

Substituting eqns. (7.30), (7.31) <strong>and</strong> (7.32) into eqn. (7.30) we get<br />

(7.30)<br />

(7.31)<br />

(7.32)<br />

(7.33)<br />

(7.34)<br />

Exercise. Determine rE assuming that b¢ 2 = 0, s = 0.9, h I = 0.8, p r = 4 <strong>and</strong> g = 1.4.<br />

N.B. It is very convenient to assume that Figures 7.13 <strong>and</strong> 7.14 can be used to derive<br />

the values <strong>of</strong> the Mach numbers Mu <strong>and</strong> M2. From Figure 7.13 we get Mu = 1.3 <strong>and</strong><br />

from Figure 7.14, M2 = 1.117. Substituting values into eqn. (7.34),<br />

1 Ê 1. 117ˆ<br />

rE =<br />

2¥ 0. 9Ë<br />

13 . ¯<br />

2<br />

Centrifugal Pumps, Fans <strong>and</strong> Compressors 235<br />

È 1<br />

+ ( - )<br />

˘<br />

1 4 1<br />

ÎÍ 08 ˚˙<br />

=<br />

1+ ¥<br />

1<br />

135 .<br />

.<br />

0. 5276<br />

2 1. 117<br />

5<br />

Calculations <strong>of</strong> r E at other pressure ratios <strong>and</strong> sweepback angles show that its value<br />

remains about 0.52 provided that s <strong>and</strong> h1 do not change.<br />

EXAMPLE 7.4. Air at a stagnation temperature <strong>of</strong> 22°C enters the impeller <strong>of</strong> a centrifugal<br />

compressor in the axial direction. The rotor, which has 17 radial vanes, rotates

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