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Treatment of the tip flow

   figure199
Figure 13:   Local flow at the blade tip as treated in THPUF-3A.
Figure 12:   Local flow at the blade tip with a developed vortex cavity.

The flow at the tip of a blade in the presence of a developed tip vortex cavity is depicted in Figure 12. The flow angularity (i.e. the contraction angle tex2html_wrap_inline792 with respect to the pure helical direction) should be included in the dynamic boundary condition in THPUF-3A. The analysis is an extension of that in [18], and is also depicted in Figure 13.

Defining as:

Then:

eqnarray221

where A is the Lighthill leading edge correction factor applied along the normal to the blade leading edge line:

equation225

By using tex2html_wrap_inline822 we get:

equation228

Finally, from tex2html_wrap_inline824 , we get:

  equation231

where tex2html_wrap_inline826 is defined as follows:

equation238

Notice that equation (7) is in a similar form to that of equation (44) in [18]

The effect of the angle tex2html_wrap_inline792 on the cavity solution at the tip and on the overall cavity volume was presented in [1] (pages 26 to 29).

The angle tex2html_wrap_inline792 can be estimated from matching the flow angle at the tip of the blade to the angle between the axial velocity tex2html_wrap_inline832 (along the trajectory of the vortex) and the total velocity direction on the surface of the tip vortex cavity. By using the following approximation on the surface of the tip vortex:

equation246

and knowing that tex2html_wrap_inline834 (see [18]) with tex2html_wrap_inline836 , we end up with:

equation250

where J is the advance coefficient.

First, the effect of including the tip flow angularity correction is given in Figure 14. Notice that the predicted cavity volume is increased appreciably when the tip effects are included.

  figure254
Figure 14:   Effect of the tip flow angularity on the cavity volume for the sample run.


next up previous
Next: About this document Up: No Title Previous: References

Spyros A. Kinnas
Sat Jun 13 10:46:17 CDT 1998