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Etude de la combustion de gaz de synthèse issus d'un processus de ...

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Chapter 3<br />

3.2.5.2 Analysis of the flow at the chamber core<br />

The whole movement has been analyzed, and an initial assessment of turbulent<br />

fluctuations was provi<strong>de</strong>d from the whole filed measurements. Specific field<br />

measurements are now exposed to evaluate the properties of turbulence in <strong>de</strong>tail. The<br />

turbulent characteristics are evaluated thanks to PIV measurements with time<br />

resolution of 5 kHz along one field of 13x13 mm and image resolution of 512x512<br />

pixels. The investigated zone is close to the center of the chamber (1.5 mm to the left),<br />

where the mean and fluctuating velocities remain re<strong>la</strong>tively elevated along a 10 ms<br />

period after TDC. Figure 3.15 shows the fluctuation velocity components in this zone.<br />

tel-00623090, version 1 - 13 Sep 2011<br />

Figure 3.15 – Time evolution of the space speed fluctuations variation (reprinted from Strozzi,<br />

2008). The zone 1 corresponds to the bottom left corner of PIV field, and the zone 4<br />

corresponds to the entire field.<br />

It is observed that both velocity components fluctuations <strong>de</strong>crease after TDC with<br />

simi<strong>la</strong>r amplitu<strong>de</strong>. The kinetic energy is evaluated only from two velocity components<br />

as follows:<br />

' 2 ' 2<br />

= + (3.10)<br />

k u v<br />

It is therefore, slightly un<strong>de</strong>restimated (~20%) due to the <strong>la</strong>ck of the third component.<br />

81

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