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

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Chapter 4<br />

variation of the normalized burning velocity of updraft syngas with the Karlovitz number<br />

is linear. From Fig. 4.21 one can see that the variation of the normalized burning<br />

velocity of downdraft syngas with the Karlovitz number is generally linear and quasilinear<br />

for φ=0.8. From Fig. 4.22 one can see that the variation of the normalized<br />

burning velocity of fluidized bed syngas with the Karlovitz number is linear for φ=0.8<br />

and quasi-linear for φ =1.0.<br />

2.0<br />

Su/S 0 u<br />

1.8<br />

1.6<br />

1.4<br />

φ<br />

1.2<br />

1.0<br />

0.8<br />

0.6<br />

1.2<br />

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

1.0<br />

0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40<br />

Karlovitz Number<br />

Figure 4.20 – Evolution of the <strong>la</strong>minar burning velocity versus Karlovitz number for updraft<br />

syngas-air mixture at different equivalence ratios and 1.0 bar.<br />

Su/S 0 u<br />

1.4<br />

1.3<br />

1.2<br />

1.1<br />

φ<br />

1.2<br />

1.0<br />

0.8<br />

0.6<br />

1.0<br />

0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40<br />

Karlovitz Number<br />

Figure 4.21 – Evolution of the <strong>la</strong>minar burning velocity versus Karlovitz number for downdraft<br />

syngas-air mixture at different equivalence ratios and 1.0 bar.<br />

107

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