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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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Centrifugal Pumps, Fans <strong>and</strong> Compressors 225<br />

FIG. 7.10. Logarithmic spiral vane. Vane angle b¢ is constant for all radii.<br />

Wislicenus (1947) <strong>and</strong> Stanitz (1952) mentioned earlier. The volume <strong>of</strong> mathematical<br />

work required to describe these theories is too extensive to justify inclusion here <strong>and</strong><br />

only a brief outline <strong>of</strong> the results is presented.<br />

Busemann’s theory applies to the special case <strong>of</strong> two-dimensional vanes curved as<br />

logarithmic spirals as shown in Figure 7.10. Considering the geometry <strong>of</strong> the vane<br />

element shown it should be an easy task for the student to prove that<br />

that the ratio <strong>of</strong> vane length to equivalent blade pitch is<br />

<strong>and</strong> that the equivalent pitch is<br />

(7.17a)<br />

(7.17b)<br />

The equi-angular or logarithmic spiral is the simplest form <strong>of</strong> radial vane system <strong>and</strong><br />

has been frequently used for pump impellers in the past. The Busemann slip factor can<br />

be written as<br />

(7.16)<br />

where both A <strong>and</strong> B are functions <strong>of</strong> r2/r1, b¢2 <strong>and</strong> Z. For typical pump <strong>and</strong> compressor<br />

impellers the dependence <strong>of</strong> A <strong>and</strong> B on r 2/r1 is negligible when the equivalent l/s<br />

exceeds unity. From eqn. (7.17b) the requirement for l/s 1, is that the radius ratio<br />

must be sufficiently large, i.e.<br />

(7.17c)

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