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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

The velocity triangles are symmetrical, so that a 2 = b 3. Also, R = N = a 2 = 68.2°,<br />

This value appears to be the same as the peak value <strong>of</strong> the efficiency curve DW/U 2<br />

= 1.0, in Figure 4.4.<br />

Stage reaction<br />

The classification <strong>of</strong> different types <strong>of</strong> axial turbine is more conveniently described<br />

by the degree <strong>of</strong> reaction, or reaction ratio R, <strong>of</strong> each stage rather than by the ratio<br />

cy2/U. As a means <strong>of</strong> description the term reaction has certain inherent advantages which<br />

become apparent later. Several definitions <strong>of</strong> reaction are available; the classical definition<br />

is given as the ratio <strong>of</strong> the static pressure drop in the rotor to the static pressure<br />

drop in the stage. However, it is more useful to define the reaction ratio as the static<br />

enthalpy drop in the rotor to the static enthalpy drop in the stage because it then<br />

becomes, in effect, a statement <strong>of</strong> the stage flow geometry. Thus,<br />

If the stage is normal (i.e. c1 = c3), then<br />

Using eqn. (4.4), h2 - h 3 = 1 – 2 (w 3 2 + w2 2 ) <strong>and</strong> eqn. (4.18) gives<br />

Assuming constant axial velocity through the stage<br />

since, upon referring to Figure 4.1, it is seen that<br />

Thus,<br />

(4.17)<br />

(4.18)<br />

(4.19)<br />

(4.20)<br />

(4.21)<br />

(4.22a)

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