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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

Incidence angle, i deg<br />

20<br />

10<br />

0.4 0.6 0.8 1.0<br />

Slip factor<br />

Introduction<br />

n = 0<br />

n = 1<br />

n = 2<br />

n = -1<br />

(a) Radius ratio, r/r 1s<br />

0<br />

0.4 0.6 0.8 1.0<br />

Even under ideal (frictionless) conditions the relative flow leaving the impeller <strong>of</strong> a<br />

compressor or pump will receive less than perfect guidance from the vanes <strong>and</strong> the flow<br />

is said to slip. If the impeller could be imagined as being made with an infinite number<br />

<strong>of</strong> infinitesimally thin vanes, then an ideal flow would be perfectly guided by the vanes<br />

<strong>and</strong> would leave the impeller at the vane angle. Figure 7.7 compares the relative flow<br />

angle, b2, obtained with a finite number <strong>of</strong> vanes, with the vane angle, b¢2. A slip factor<br />

may be defined as<br />

Absolute flow angle, a 1 deg<br />

40<br />

20<br />

n = 0<br />

n = -1<br />

n = 1<br />

n = 2<br />

(b) Radius ratio, r/r 1s<br />

FIG. 7.6. Effect <strong>of</strong> prewhirl vanes on flow angle <strong>and</strong> incidence for a1s = 30deg, b1s =<br />

60deg <strong>and</strong> b ¢ 1s = 60deg. (a) Incidence angle; (b) Inducer flow angle.<br />

C r2<br />

C qs<br />

b¢ 2<br />

W 2<br />

b 2<br />

U 2<br />

C ¢ q2<br />

C 2<br />

C q2<br />

b 2¢ is the vane angle<br />

b 2 is the average<br />

relative flow angle<br />

FIG. 7.7. Actual <strong>and</strong> hypothetical velocity diagrams at exit from an impeller with back<br />

swept vanes.

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