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Handbook of Turbomachinery Second Edition Revised - Ventech!

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Figure 26 Velocity triangle <strong>of</strong> steam through a steam turbine stage.<br />

steam expanded from the pressure upstream <strong>of</strong> a stage to the downstream<br />

pressure without losses.<br />

The velocity <strong>of</strong> the rotating blades or wheel velocity, is designated W,<br />

and the vector result <strong>of</strong> V1 and W is the velocity <strong>of</strong> the entering steam<br />

relative to the rotating blade, V2. a is the angle at which the steam leaves the<br />

stationary blade relative to the plane <strong>of</strong> rotation <strong>of</strong> the rotating blade. a is<br />

sometimes referred to as the ‘‘nozzle angle’’ although it is actually the steam<br />

angle and typically about 28 larger than the nozzle passage angle.<br />

In an impulse design, there is little pressure drop across the rotating<br />

blades so that the relative velocity leaving the rotating blade, V3 (Fig. 26),<br />

would be equal to the entering velocity V2 if there were no frictional losses.<br />

The absolute velocity <strong>of</strong> the exiting steam is V4, the vector sum <strong>of</strong> V3 and the<br />

wheel speed, W. A goal <strong>of</strong> the stage design process is to have the direction <strong>of</strong><br />

the flow at exit be as close as possible to axial for entry into the next stage<br />

[9].<br />

The force on the blade is proportional to the change in tangential<br />

components <strong>of</strong> the velocity, i.e., the entering tangential velocity, Va, less the<br />

exit tangential velocity, Vb.<br />

Copyright © 2003 Marcel Dekker, Inc.

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