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690 Chapter 12 ■ Turbomachines<br />

usually of the axial-flow type. Often they are multistage turbomachines, although single-stage compressible<br />

turbines are also produced. They may be either an impulse type or a reaction type. With<br />

compressible flow turbines, the ratio of static enthalpy or temperature drop across the rotor to this<br />

drop across the stage, rather than the ratio of static pressure differences, is used to determine reaction.<br />

Strict impulse 1zero pressure drop2 turbines have slightly negative reaction; the static enthalpy<br />

or temperature actually increases across the rotor. Zero-reaction turbines involve no change<br />

of static enthalpy or temperature across the rotor but do involve a slight pressure drop.<br />

A two-stage, axial-flow impulse turbine is shown in Fig. 12.38a. The gas accelerates through<br />

the supply nozzles, has some of its energy removed by the first-stage rotor blades, accelerates again<br />

through the second-stage nozzle row, and has additional energy removed by the second-stage rotor<br />

blades. As shown in Fig. 12.38b, the static pressure remains constant across the rotor rows.<br />

Across the second-stage nozzle row, the static pressure decreases, absolute velocity increases, and<br />

the stagnation enthalpy 1temperature2 is constant. Flow across the second rotor is similar to flow<br />

across the first rotor. Since the working <strong>fluid</strong> is a gas, the significant decrease in static pressure<br />

across the turbine results in a significant decrease in density—the flow is compressible. Hence,<br />

more detailed analysis of this flow must incorporate various compressible flow concepts developed<br />

in Chapter 11. Interesting phenomena such as shock waves and choking due to sonic conditions at<br />

the “throat” of the flow passage between blades can occur because of compressibility effects. The<br />

interested reader is encouraged to consult the various references available 1e.g., Refs. 2, 3, 202 for<br />

fascinating applications of compressible flow principles in turbines.<br />

The rotor and nozzle blades in a three-stage, axial-flow reaction turbine are shown in Fig.<br />

12.39a. The axial variations of pressure and velocity are shown in Fig. 12.39c. Both the stationary<br />

and rotor blade 1passages2 act as flow-accelerating nozzles. That is, the static pressure and enthalpy<br />

1temperature2 decrease in the direction of flow for both the fixed and the rotating blade rows.<br />

This distinguishes the reaction turbine from the impulse turbine 1see Fig. 12.38b2. Energy is removed<br />

from the <strong>fluid</strong> by the rotors only 1the stagnation enthalpy or temperature is constant across<br />

the adiabatic flow stators2.<br />

Rotor blades<br />

(Rotor)<br />

Moving<br />

blades<br />

Nozzles<br />

Moving<br />

blades<br />

(Rotor)<br />

Fixed<br />

blades<br />

(Stator)<br />

Nozzles<br />

(Stator)<br />

(a)<br />

(a)<br />

Stagnation<br />

enthalpy or<br />

temperature<br />

Static<br />

enthalpy or<br />

temperature<br />

(b)<br />

Static<br />

pressure<br />

Static<br />

pressure<br />

Absolute<br />

velocity<br />

Absolute<br />

velocity<br />

(b)<br />

F I G U R E 12.38 Enthalpy, velocity,<br />

and pressure distribution in two-stage impulse<br />

turbine.<br />

(c)<br />

F I G U R E 12.39 Enthalpy,<br />

pressure, and velocity distribution in a<br />

three-stage reaction turbine.

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