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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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Stage pressure rise<br />

Consider first the ideal compressor stage which has no stagnation pressure losses.<br />

Across the rotor row p0rel is constant <strong>and</strong> so<br />

Across the stator row p0 is constant <strong>and</strong> so<br />

(5.23a)<br />

(5.23b)<br />

Adding together the pressure rise for each row <strong>and</strong> considering a normal stage (c 3 = c1)<br />

gives<br />

(5.24)<br />

For either velocity triangle (Figure 5.2), the cosine rule gives c 2 - U 2 + w 2 = 2Uw<br />

cos(p/2 - b) or<br />

Substituting eqn. (5.25) into the stage pressure rise,<br />

Again, referring to the velocity diagram, wy1 - wy2 = cy2 - cy1 <strong>and</strong><br />

Axial-flow Compressors <strong>and</strong> Fans 155<br />

FIG. 5.6. Effect <strong>of</strong> design stage loading (yd) on simplified <strong>of</strong>f-design performance<br />

characteristics (adapted from Horlock 1958).<br />

(5.25)<br />

(5.26)<br />

It is noted that, for an isentropic process, Tds = 0 = dh - (1/r)dp <strong>and</strong>, therefore,<br />

Dh = (1/r)Dp.

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