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Handbook of Turbomachinery Second Edition Revised - Ventech!

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Projected Shape in Meridional Plane<br />

Let us first consider the shape projected by a rotor on the meridional plane,<br />

which is a plane through the axis <strong>of</strong> rotation. This shape is illustrated by the<br />

contours shown for the centrifugal impellers in Figs. 2 and 4. The<br />

boundaries <strong>of</strong> the indicated flow passage turn the flow radially outward<br />

and thereby produce additional velocity gradients normal to the stream<br />

surfaces. The velocity <strong>of</strong> a gas is higher at the casing than at the hub.<br />

Blade Shapes<br />

Refer now to Eq. (16) and note that oa must have finite values in centrifugal<br />

and mixed-flow impellers. The velocity gradients described by Eq. (17)<br />

augment those noted in the previous subsection when the magnitude <strong>of</strong> oa is<br />

less than one half <strong>of</strong> the angular velocity <strong>of</strong> the impeller. Both the vorticities<br />

and the curvatures <strong>of</strong> the hub and shroud induce high gas velocities at the<br />

outer casing and low velocities at the hub. The effect <strong>of</strong> vorticity is reversed<br />

at greater values <strong>of</strong> oa. Vorticity and the outward curvature <strong>of</strong> the flow have<br />

been responsible for stagnated flow at the hub and separated flow at the<br />

casing. Outward curvature <strong>of</strong> the hub and casing should thus be deferred<br />

until the value <strong>of</strong> oa is about 50% <strong>of</strong> the angular velocity <strong>of</strong> the rotor. For<br />

this preliminary design, one may estimate the gradients by assuming that the<br />

path <strong>of</strong> the flow follows the shape <strong>of</strong> the blades.<br />

One should strive to design the blades so that as much free vortex<br />

rotation as possible is imparted to the gas in the regions where the flow has a<br />

strong axial component. Recall, however, that mechanical stresses can limit<br />

this objective.<br />

As a tentative diffusion limit, the relative velocity at the impeller outlet<br />

should be no less than 60% <strong>of</strong> the maximum relative velocity at the inlet. If<br />

the resulting relative velocity component at the impeller outlet is<br />

uncomfortably high, the use <strong>of</strong> relative tangential velocities opposite to<br />

those <strong>of</strong> the impeller blades should be considered. The blades <strong>of</strong> such<br />

impellers are said to have backward curvature. The absolute value <strong>of</strong> the<br />

outlet tangential component <strong>of</strong> gas velocity is reduced, which lessens the<br />

task <strong>of</strong> the following stator or diffuser. Impeller cost, size, stresses, and<br />

possibly efficiency are the principal limitations to the amount <strong>of</strong> backward<br />

curvature that may be selected.<br />

Slip Factor<br />

Unfortunately, there is no good general rule for estimating the deviation<br />

angle or an equivalent angle. A quantity known as slip factor is an<br />

Copyright © 2003 Marcel Dekker, Inc.

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