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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

design in which none <strong>of</strong> its natural frequencies coincides with any excitation frequency.<br />

The subject is complex, interesting but outside <strong>of</strong> the scope <strong>of</strong> the present text.<br />

Centrifugal stresses<br />

Consider a blade rotating about an axis O as shown in Figure 4.15. For an element<br />

<strong>of</strong> the blade <strong>of</strong> length dr at radius r, at a rotational speed W the elementary centrifugal<br />

load dFc is given by<br />

where dm = rmA dr <strong>and</strong> the negative sign accounts for the direction <strong>of</strong> the stress gradient<br />

(i.e. zero stress at the blade tip to a maximum at the blade root),<br />

F c+dF c<br />

FIG. 4.15. Centrifugal forces acting on rotor blade element.<br />

F c<br />

o<br />

dr<br />

r<br />

W

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