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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

<strong>and</strong>, therefore,<br />

(7.24a)<br />

This formulation is useful if the flow angles can be specified. Alternatively, <strong>and</strong> more<br />

usefully, as cq2 = sc¢q2 = s(U2 - cr2tan b¢2), then<br />

(7.24b)<br />

where Mu = U2/a01, is now defined as a blade Mach number.<br />

It is <strong>of</strong> interest to calculate the variation <strong>of</strong> the pressure ratio <strong>of</strong> a radially vaned (b¢2<br />

= 0) centrifugal air compressor to show the influence <strong>of</strong> blade speed <strong>and</strong> efficiency on<br />

the performance. With g = 1.4 <strong>and</strong> s = 0.9 (i.e. using the Stanitz slip factor, s = 1 -<br />

1.98/Z <strong>and</strong> assuming Z = 20, the results evaluated are shown in Figure 7.12. It is clear<br />

that both the efficiency <strong>and</strong> the blade speed have a strong effect on the pressure ratio.<br />

In the 1970s the limit on blade speed due to centrifugal stress was about 500m/s <strong>and</strong><br />

FIG. 7.12. Variation <strong>of</strong> pressure ratio with blade speed for a radial-bladed compressor<br />

(b¢ 2 = 0) at various values <strong>of</strong> efficiency.

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