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Chapter 4 Vortex detection - Computer Graphics and Visualization

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4.4. The enhanced curvature centre method<br />

caused by shear flow or interacting vortices. This is illustrated by two analytical flows:<br />

a circular <strong>and</strong> an elliptic flow.<br />

circular flow<br />

The ideal test case for the curvature centres method is a circular flow. Since the streamlines<br />

are perfect concentric circles, all the curvature centres should coincide. Let the<br />

velocity field Ú Ü Ý ÚÜ Ü Ý ÚÝ Ü Ý of the circular flow be defined by<br />

Ú Ü Ý Ý Ü (4.13)<br />

Figure 4.13a depicts streamlines of this velocity field. The centripetal acceleration<br />

Ü Ý ÜÝ is given by<br />

Ü Ý ÚÜ<br />

Ý<br />

<br />

Ú<br />

Ü<br />

which results in the curvature centre Ô :<br />

Ú<br />

ÚÝ<br />

Ý <br />

Ü<br />

(4.14)<br />

<br />

Ü Ý (4.15)<br />

Ô Ô Ü Ý Ü Ý (4.16)<br />

which proves that for perfect, circular streamlines, the curvature centres coincide in<br />

the origin (0,0), as Figure 4.13b shows.<br />

elliptic flow<br />

In the case that the streamlines are not perfect circles, but deformed to ellipses, the<br />

velocity field is given by:<br />

Ú Ü Ý Ý Ü (4.17)<br />

with <strong>and</strong> . Figure 4.13c shows an example with .<br />

Then, the centripetal acceleration ÜÝ is given by<br />

Ü Ý ÚÜ<br />

which results in the curvature centres Ô :<br />

Ú Ú<br />

ÚÝ<br />

Ü Ý <br />

Ý Ü<br />

Ü<br />

Ü<br />

<br />

<br />

Ý<br />

Ý<br />

<br />

<br />

(4.18)<br />

(4.19)<br />

(4.20)<br />

Ô Ô Ü Ý Ü Ý Ü Ý (4.21)<br />

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