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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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P S P S<br />

c 2<br />

Direction<br />

<strong>of</strong> rotation<br />

(a)<br />

(b)<br />

Radial Flow Gas Turbines 259<br />

a 2 b 2<br />

U 2<br />

FIG. 8.5. Optimum flow condition at inlet to the rotor. (a) Streamline flow at rotor inlet;<br />

p is for pressure surface, s is for suction surface. (b) Velocity diagram for the<br />

pitchwise averaged flow.<br />

Figure 8.5b indicates the average relative velocity w2, entering the rotor at angle b2<br />

<strong>and</strong> giving optimum flow conditions at the vane leading edge. As the rotor vanes in<br />

IFR turbines are assumed to be radial, the angle b2 is an angle <strong>of</strong> incidence, <strong>and</strong> as<br />

drawn it is numerically positive. Depending upon the number <strong>of</strong> rotor vanes this angle<br />

may be between 20 <strong>and</strong> 40deg. The static pressure gradient across the passage causes<br />

a streamline shift <strong>of</strong> the flow towards the suction surface. Streamfunction analyses <strong>of</strong><br />

this flow condition show that the streamline pattern properly locates the inlet stagnation<br />

point on the vane leading edge so that this streamline is approximately radial (see<br />

Figure 8.5a). It is reasoned that only at this flow condition will the fluid move smoothly<br />

into the rotor passage. Thus, it is the averaged relative flow that is at an angle <strong>of</strong> incidence<br />

b2 to the vane. Whitfield <strong>and</strong> Baines (1990) have comprehensively reviewed<br />

computational methods used in determining turbomachinery flows, including<br />

streamfunction methods.<br />

Wilson <strong>and</strong> Jansen (1965) appear to have been the first to note that the optimum<br />

angle <strong>of</strong> incidence was virtually identical to the angle <strong>of</strong> “slip” <strong>of</strong> the flow leaving the<br />

w 2

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