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

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Experimental and numerical <strong>la</strong>minar syngas <strong>combustion</strong><br />

4.1.1.4 Laminar burning velocity<br />

Fig. 4.18 gives the stretched <strong>la</strong>minar burning velocity versus the f<strong>la</strong>me stretch rate for<br />

typical syngas compositions.<br />

The maximum value <strong>la</strong>minar burning velocity is presented at the stoichiometric<br />

equivalence ratio, while lean or rich mixtures <strong>de</strong>crease the burning velocities.<br />

Downdraft syngas composition shows the highest burning velocities for all the<br />

equivalence ratios consi<strong>de</strong>red. The stretched burning velocity increases with the<br />

increase of f<strong>la</strong>me stretch rate for lean (φ=0.8) syngas-air mixtures. This behavior<br />

remains for stoichiometric and rich (φ=1.2) mixtures in the case of updraft and<br />

downdraft compositions. In opposite, burning velocity <strong>de</strong>creases with the increase of<br />

stretch rate for stoichiometric fluidized syngas-air case.<br />

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

Su (m/s)<br />

0.4<br />

φ =0.6<br />

0.3<br />

0.2<br />

0.1<br />

Updraft<br />

Downdraft<br />

0.0<br />

0 50 100 150 200 250 300 350 400<br />

κ (s -1 )<br />

0.5<br />

φ =0.8<br />

0.4<br />

Su (m/s)<br />

0.3<br />

0.2<br />

0.1<br />

0.0<br />

Updraft<br />

Dow ndraft<br />

Fluidized<br />

0 100 200 300 400 500 600<br />

κ (s -1 )<br />

Figure 4.18a – Stretched burning velocity versus stretch rate for syngas-air mixtures at various<br />

equivalence ratios.<br />

104

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