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

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Experimental study of engine-like turbulent <strong>combustion</strong><br />

single compression experiments performed enables to <strong>de</strong>fine a typical scattering on<br />

less than 4.0 mm (from -13 mm to -17 mm).<br />

The TDC position has also some scattering but only of 1 mm (from 419 mm to 420 mm)<br />

which could be endorsed to some mechanical <strong>de</strong>formation imposed by elevated incylin<strong>de</strong>r<br />

pressures. Consi<strong>de</strong>ring a piston stroke of 419 mm, the overall uncertainty of<br />

the piston initial position is lower than 1.0%. This jitter on the initial position can be<br />

converted to time scale by consi<strong>de</strong>ring the average piston speed of 9.5 m/s. This<br />

conversion gives a maximum value of 0.42 ms.<br />

Consi<strong>de</strong>ring that the volume insi<strong>de</strong> the chamber is obtained from the piston position,<br />

the influence of this jitter on the piston position from one experiment to another is then<br />

analyzed in figure 5.3 for the case of updraft syngas without <strong>combustion</strong> in or<strong>de</strong>r to<br />

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

avoid the effect of the spark time scattering. The choice of the same fuel also avoids<br />

differences in the polytropic coefficient of the mixture being compressed.<br />

In the case shown in the figure 5.3, the difference in the initial piston position is 1.75<br />

mm. It is observed that there is no significant difference on the piston position along<br />

time.<br />

450<br />

Piston position (mm)<br />

360<br />

270<br />

180<br />

90<br />

0<br />

90 100 110 120 130 140<br />

Time (ms)<br />

Figure 5.3- Piston disp<strong>la</strong>cement during single compression of updraft syngas-air.<br />

From figure 5.3 it is also observed the evolution in a “stair” mo<strong>de</strong> of the <strong>la</strong>ser piston<br />

position signal. As the in-cylin<strong>de</strong>r volume variation is obtained from this signal,<br />

therefore a peak <strong>de</strong>tection filter was applied to this signal (figure 5.4).<br />

142

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