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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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decrease with the addition <strong>of</strong> further stages to the turbine. One <strong>of</strong> the earliest attempts<br />

to assess the flow variation <strong>of</strong> a multistage turbine is credited to Stodola (1945), who<br />

formulated the much used “ellipse law”. The curve labelled “multistage” in Figure 4.21<br />

is in agreement with the “ellipse law” expression<br />

[ ]<br />

( ) = -( )<br />

2<br />

÷ 01 0 0 0<br />

12<br />

I II I ,<br />

m T p k 1 p p<br />

Axial-flow Turbines: Two-dimensional Theory 123<br />

FIG. 4.21. Turbine flow characteristics (after Mallinson <strong>and</strong> Lewis 1948).<br />

(4.32)<br />

where k is a constant.<br />

This expression has been used for many years in steam turbine practice, but an accurate<br />

estimate <strong>of</strong> the variation in swallowing capacity with pressure ratio is <strong>of</strong> even<br />

greater importance in gas turbine technology. Whereas the average condensing steam<br />

turbine, even at part-load, operates at very high pressure ratios, some gas turbines may<br />

work at rather low pressure ratios, making flow matching with a compressor a difficult<br />

problem. The constant value <strong>of</strong> swallowing capacity, reached by the single-stage turbine<br />

at a pressure ratio a little above 2, <strong>and</strong> the other turbines at progressively higher pressure<br />

ratios, is associated with choking (sonic) conditions in the turbine stator blades.<br />

Flow characteristics <strong>of</strong> a multistage turbine<br />

Several derivations <strong>of</strong> the ellipse law are available in the literature. The derivation<br />

given below is a slightly amplified version <strong>of</strong> the pro<strong>of</strong> given by Horlock (1958). A<br />

more general method has been given by Egli (1936) which takes into consideration the<br />

effects when operating outside the normal low loss region <strong>of</strong> the blade rows.<br />

Consider a turbine comprising a large number <strong>of</strong> normal stages, each <strong>of</strong> 50% reaction;<br />

then, referring to the velocity diagram <strong>of</strong> Figure 4.22a, c 1 = c3 = w2 <strong>and</strong> c2 = w3.<br />

If the blade speed is maintained constant <strong>and</strong> the mass flow is reduced, the fluid angles

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