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24 S. Men<strong>de</strong>z and F. Nicoud<br />

Figure 16. Isosurface of Q criterion (5 V j 2 /d 2 ) from Run C showing the instantaneous flow<br />

structure. Top: top view. Bottom: si<strong>de</strong> view.<br />

fields. Note that they appear beneath the location where the vortices composing the CVP<br />

g<strong>et</strong> closer from each other, at approximately x = 3.5 d.<br />

Instantaneous fields of Q-criterion offer a very different picture of the vortical flow<br />

structure. Instantaneous structures are much intense, as shown in figure 16, where an<br />

instantaneous iso-surface of Q-criterion at 5 V j 2 /d 2 is shown. Again, the solid wall is<br />

partly transparent to allow observation of the in-hole behaviour. The instantaneous field<br />

is dominated by shear layer vortices formed at the upstream face of the j<strong>et</strong> and also<br />

insi<strong>de</strong> the aperture, at the high shear zone that separates the low-momentum and the<br />

j<strong>et</strong>ting regions. These in-hole vortices have an hairpin form with two legs located in the<br />

low-momentum region, in the direction of the hole. The counter-rotating vortex pair<br />

observed within the hole in the average field actually results from the averaging of series<br />

of hairpin vortices: they form a unique structure in an instantaneous visualisation. The<br />

hairpin vortices seem to result from the roll-up of the vorticity located at the sharp edge<br />

of the hole entrance. Outsi<strong>de</strong> the hole, in addition to the shear layer vortices, another<br />

type of vortices are d<strong>et</strong>ected. They are located close to the wall and have a streamwise

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