Flow over a Magnetically Suspended Cylinder in an Axial Free Stream
Flow over a Magnetically Suspended Cylinder in an Axial Free Stream
Flow over a Magnetically Suspended Cylinder in an Axial Free Stream
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Fig. 2(a) A magnetically supported 45mm diameter cyl<strong>in</strong>der model<br />
Fig. 2(b) A magnetically supported 85mm diameter cyl<strong>in</strong>der model<br />
III. Results <strong>an</strong>d Discussion<br />
A. Wake beh<strong>in</strong>d magnetically supported cyl<strong>in</strong>der<br />
The me<strong>an</strong> velocity distribution beh<strong>in</strong>d the L/D=5.02 model is presented <strong>in</strong> both vertical (z) <strong>an</strong>d horizontal (y)<br />
directions <strong>in</strong> Fig. 3. The dist<strong>an</strong>ce is measured from the trail<strong>in</strong>g edge of the model. An earlier test employed the PIV<br />
system on lo<strong>an</strong> <strong>an</strong>d the results <strong>in</strong>dicated excellent results <strong>in</strong> the wake while limit<strong>in</strong>g the illum<strong>in</strong>ation away from the<br />
position sens<strong>in</strong>g cameras. Results from <strong>an</strong>other PIV measurement <strong>in</strong> water will be also discussed oater. However, these<br />
velocity measurements relied on a more conventional total head probe as well as a hot-wire probe. Naturally, the<br />
results are limited to regions where these <strong>in</strong>strumentations are applicable. Figure 3 nonetheless demonstrates excellent<br />
flow axisymmetry measured with the total head probe. The results clearly benefited from the absence of the model<br />
support <strong>in</strong> the present system. The symmetry of the flow <strong>an</strong>d the repeatability of the measurements are further<br />
illustrated <strong>in</strong> Fig. 4 by vertical <strong>an</strong>d horizontal probe traverses.<br />
- 3 –<br />
Americ<strong>an</strong> Institute of Aeronautics <strong>an</strong>d Astronautics